Abstract: CERN-LHC. We present ALICE results on transverse momentum ($p_{\rm T}$) and rapidity ($y$) differential production cross sections, mean transverse momentum and mean transverse momentum square of inclusive $J/\psi$ and $\psi(2S)$ at forward rapidity (2.5 < $y$ < 4) as well as $\psi(2S)$-to-$J/\psi$ cross section ratios. These quantities are measured in pp collisions at center of mass energies $\sqrt{s}$ = 5.02 and 13 TeV. Both charmonium states are reconstructed in the dimuon decay channel, using ALICE muon spectrometer.

Energy dependence of forward-rapidity J/$\psi$ and $\psi(2S)$ production in pp collisions at the LHC;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. Electrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy $\sqrt{s_{\rm NN}}=2.76$ TeV. The transverse momentum ($p_{\rm T}$) differential production yields at mid-rapidity were used to calculate the nuclear modification factor $R_{\rm AA}$ in the interval $3<~p_{\rm T}<~ 18$ GeV/$c$. The $R_{\rm AA}$ shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed.

Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. Measurements of multi-particle azimuthal correlations (cumulants) for charged particles in p-Pb at sqrt{s_{NN}}=5.02 TeV and Pb-Pb at sqrt{s_{NN}}=2.76 TeV collisions are presented. They help address a question if there is evidence for global, flow-like, azimuthal correlations in the p-Pb system. Comparisons are made to measurements from the larger Pb-Pb system, where such evidence is established. In particular, the second harmonic two-particle cumulants are found to decrease with multiplicity, characteristic of a dominance of few-particle correlations in p-Pb collisions. However, when a |delta eta| gap is placed to suppress such correlations, the two-particle cumulants begin to rise at high-multiplicity, indicating the presence of global azimuthal correlations. The Pb-Pb values are higher than the p-Pb values at similar multiplicities. In both systems, the second harmonic four-particle cumulants exhibit a transition from positive to negative values when the multiplicity increases. The negative values allow for a measurement of v2{4} to be made, which is found to be higher in Pb-Pb collisions at similar multiplicities. The second harmonic six-particle cumulants are also found to be higher in Pb-Pb collisions. In Pb-Pb collisions, we generally find v2{4}~=v2{6}!=0 which is indicative of a Bessel-Gaussian function for the v2 distribution. For very high-multiplicity Pb-Pb collisions, we observe that the four- and six-particle cumulants become consistent with 0. Finally, third harmonic two-particle cumulants in p-Pb and Pb-Pb are measured. These are found to be similar for overlapping multiplicities, when a |delta eta|>1.4 gap is placed.

Multi-particle azimuthal correlations in p-Pb and Pb-Pb collisions at the LHC;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurement of the inclusive Psi(2S) production in p-Pb collisions at sqrt(s_NN)=5.02TeV at CERN LHC. The measurements are performed at forward (2.03

Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurement of the two-pion three-dimensional femtoscopy in p-Pb collisions at a center-of-mass energy of 5.02 TeV. Femtoscopic radii are obtained in as a function of four multiplicity event classes and seven pair transverse momentum ranges. The measured p-Pb radii, at high multiplicity and low pair transverse momentum, are 10-20% higher than those observed in pp collisions but below those ones observed in A-A collisions.

Two-pion femtoscopy in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2016;HEPData


Abstract:
CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ > 30 GeV, |$\eta$| < 1.444 or 1.56 < |$\eta$| < 2.5
- $\mu$: $p_\text{T}$ > 30 GeV, |$\eta$| < 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ > 50 GeV, |$\eta$| < 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) > 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ > 30 GeV, |$\eta$| < 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) > 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) > 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) > 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).

Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. The measurement of primary $\pi^{\pm}$, K$^{\pm}$, p and $\overline{p}$ production at mid-rapidity ($|y| <$ 0.5) in proton-proton collisions at $\sqrt{s} = 7$ TeV performed with ALICE (A Large Ion Collider Experiment) at the Large Hadron Collider (LHC) is reported. Particle identification is performed using the specific ionization energy loss and time-of-flight information, the ring-imaging Cherenkov technique and the kink-topology identification of weak decays of charged kaons. Transverse momentum spectra are measured from 0.1 up to 3 GeV/$c$ for pions, from 0.2 up to 6 GeV/$c$ for kaons and from 0.3 up to 6 GeV/$c$ for protons. The measured spectra and particle ratios are compared with QCD-inspired models, tuned to reproduce also the earlier measurements performed at the LHC. Furthermore, the integrated particle yields and ratios as well as the average transverse momenta are compared with results at lower collision energies.

Measurement of pion, kaon and proton production in proton-proton collisions at $\sqrt{s}=7$ TeV;ALICE Collaboration;2017;HEPData


Abstract:
CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.

Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract:
CERN-LHC. A search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks is presented. Events with one charged lepton (electron or muon) and at least five jets, or two oppositely charged leptons (electron-electron, muon-muon, electron-muon) and at least four jets, are selected from a data sample corresponding to an integrated luminosity of 19.5 invfb collected by the CMS experiment at the LHC in pp collisions at a centre-of-mass energy of 8 TeV.

Leptons are defined by:
- ptLepton > 30 (20) GeV for the single lepton (dilepton) channel
- |etaLepton| < 2.1 (2.5) for muons (electrons)
- sum of travserse momentum of particles within dR < 0.4 of the lepton direction < 10% of ptLepton.

Jets are defined by clustering particle-flow particles using the anti-kT algorithm with radius R=0.5 and are required to have:
- ptJet > 30 GeV
- |etaJet| < 2.5.
The CSV algorithm is used to assign a b tagging score to each jet.

In order to separate the signal from the larger ttbar+jets background, this analysis uses a matrix element method that assigns a probability density value to each reconstructed event under signal or background hypotheses.

The ratio between the two values is used in a maximum likelihood fit to extract the signal yield. The results are presented in terms of the measured signal strength modifier, mu, relative to the standard model prediction for a Higgs boson mass of 125 GeV. The observed (expected) exclusion limit at a 95% confidence level is mu < 4.2 (3.3), corresponding to a best fit value of 1.2 +1.6,-1.5.

Search for a Standard Model Higgs Boson Produced in Association with a Top-Quark Pair and Decaying to Bottom Quarks Using a Matrix Element Method;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. The normalized differential cross section for top quark pair (ttbar) production is measured in pp collisions at a centre-of-mass energy of 8 TeV at the CERN LHC using the CMS detector in data corresponding to an integrated luminosity of 19.7 inverse femtobarns. The measurements are performed in the lepton+jets (e/mu+jets) and in the dilepton (e e, mu mu, and e mu) decay channels. The ttbar cross section is measured as a function of the kinematic properties of the charged leptons, the jets associated to b quarks, the top quarks, and the ttbar system. The data are compared with several predictions from perturbative QCD up to approximate next-to-next-to-leading-order precision. No significant deviations are observed relative to the standard model predictions.

Measurement of the differential cross section for top quark pair production in pp collisions at sqrt(s) = 8 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. The charged-particle pseudorapidity density distribution is measured for different centralities of Pb Pb collisions at $\sqrt{s}$/nucleon-pair of 2760 GeV. From this the total number of produced charged particles is calculated versus the number of participating nucleons along with the pseudorapidity density of charged particles per participant pair versus the number of participating nucleons for different eta ranges. Finally the distribution is converted to the charged-particle rapidity density distribution to extract the width of the distribution and compare it to lower energy data. UPDATE(15/07/2015):typo correction; 20-30%, 30-40% labels changed to 10-20, 20-30% on first table.

Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurements of the double-differential Drell-Yan cross sections are presented using an integrated luminosity of 19.7 inverse femtobarns in the dimuon channel of proton-proton collision data recorded in 2012 with the CMS detector at the LHC at sqrt(s) = 8 TeV. Covariance matrices are provided in addition to the tables given in the paper.

Measurement of the Z boson differential cross section in transverse momentum and rapidity in proton-proton collisions at 8 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. Prompt D meson and non-prompt JPSI yields are studied as a function of the multiplicity of charged particles produced in inelastic proton-proton collisions at a centre-of-mass energy of SQRT(S) = 7 TeV. The results are reported as a ratio between yields in a given multiplicity interval normalised to the multiplicity-integrated ones (relative yields). They are shown as a function of the multiplicity of charged particles normalised to the average value for inelastic collisions (relative charged-particle multiplicity). D$^{0}$, D$^{+}$ and D*$^{+}$ mesons are measured in five PT intervals from 1 GeV/c to 20 GeV/c and for |YRAP| < 0.5 via their hadronic decays. The D0-meson relative yield is also measured as a function of the relative multiplicity at forward pseudo-rapidity. The non-prompt JPSI i.e. the B hadron, contribution to the inclusive JPSI production is measured in the di-electron decay channel at central rapidity. It is evaluated for PT > 1.3 GeV/c and |YRAP| < 0.9, and extrapolated to PT > 0.

Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at $\mathbf{\sqrt{{\textit s}}}=7$ TeV;ALICE Collaboration;2016;HEPData


Abstract:
CERN-LHC. The top quark pair production cross section is measured for the first time in proton-proton collisions at sqrt(s) = 13 TeV by the CMS experiment at the CERN LHC, using data corresponding to an integrated luminosity of 43 inverse picobarns. The measurement is performed by analyzing events with at least one electron and one muon of opposite charge, and at least two jets. The measured cross section is 746 +/- 58 (stat) +/- 53 (syst) +/- 36 (lum) pb, in agreement with the expectation from the standard model.

UPDATE (16 MAY 2017): revise measurement to match published version (arXiv:1510.05302v3).

Measurement of the top quark pair production cross section in proton-proton collisions at sqrt(s)=13 TeV;CMS Collaboration;2017;HEPData


Abstract:
CERN-LHC. The r3 variable is measured with charged pions in Pb-Pb collisions at the LHC. The following measurements are reported:
- C2 for same- and mixed-charge pairs versus qinv for six kT intervals and two centrality intervals.
- C2 fit parameters: lambda and Rch
- C3 and c3 for same- and mixed-charge triplets versus Q3 in two KT3 intervals and six centrality intervals.
- r3 versus Q3 in two different KT3 intervals and six different centrality intervals.

Two and Three-Pion Quantum Statistics Correlations in Pb-Pb Collisions at sqrt(sNN)=2.76 TeV at the LHC;ALICE Collaboration;2016;HEPData


Abstract:
CERN-LHC. Measurements of the ZZ production cross section in proton-proton collisions at center-of-mass energies of 7 and 8 TeV are presented.
Candidate events for the leptonic decay mode ZZ->2l2nu, where l denotes an electron or a muon, are reconstructed and selected from data corresponding to an integrated luminosity of 5.1 (19.6)/fb at 7 (8) TeV collected with the CMS experiment.
The selected data are analyzed to search for anomalous triple gauge couplings involving the ZZ final state. These limits are then combined with the previously published CMS results for ZZ in 4l final states.

We define a reduced missing transverse energy (reduced-MET) variable:
- The transverse momenta (pT) of all the individual particle candidates in the event and of the clustered jets are decomposed along an orthogonal set of
 axes in the transverse plane of the detector. One of the axes is
 defined by the pT of the charged dilepton system (pT(ll)), the other perpendicular to it. - We define the recoil of the l+l' system in two different
ways: (1) the clustered recoil (Rc) is the vectorial sum of the
momenta of the jets reconstructed in the event (2) the unclustered recoil (Ru) is the vectorial sum of the transverse momenta of all particle candidates in
the event, with the exception of the two leptons. - On each
axis (i = parallel/orthogonal to the dilepton system pT), the reduced MET projection is defined as:
reduced-MET_i = - pT(ll)_i - Rc/u_i, where Rc/u_i
represents the choice of Rc or Ru that minimizes the absolute value
of that reduced-MET component, and pT(ll)_i is a projection of the transverse momentum of the Z boson.
- The absolute reduced-MET variable is the sum in quadrature of the two components.
Selection is defined as: - 2l (l=e+,e-,mu+,mu-). No opposite charge sign is required.
- pT(mu) > 20 GeV; |eta(mu)| < 2.4
- pT(e) > 20 GeV; |eta(e)| < 2.5
- Jet: particle-flow (PF) candidates, using the anti-kT algorithm with a distance parameter of 0.5 (pT > 20 GeV).
- |Dilepton invariant mass - 91| < 7.5 GeV
- pT(ll) > 45 GeV
- Events containing jets with pT > 20 GeV and identified as b-quark jets are rejected
- Events containing jets with pT > 30 GeV are rejected
- Reduced-MET > 65 GeV
- 0.4 > MET/pT(ll) > 1.8
- DeltaPhi(MET,jet) > 0.5 rad
- DeltaPhi(MET,lepton) > 0.2 rad
- Events containing additional leptons with pT > 10 GeV (electron) or 3 GeV (muon) are rejected.

Measurements of the ZZ production cross sections in the 2 l 2 nu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV and combined constraints on triple gauge couplings;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. A search for neutral Higgs bosons predicted in the minimal supersymmetric standard model (MSSM) for $\mu^{+} \mu^{-}$ decay channels is presented. The analysis uses data collected by the CMS experiment at the LHC in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV, corresponding to integrated luminosities of 5.1 and 19.3 fb$^{-1}$, respectively. The search is sensitive to Higgs bosons produced through the gluon fusion process and in association with a bb quark pair. No statistically significant excess is observed in the $\mu^{+} \mu^{-}$ mass spectrum. Results are interpreted in the framework of several benchmark scenarios, and the data are used to set an upper limit on the MSSM parameter $ \tan{ \beta} $ as a function of the mass of the pseudoscalar A boson in the range from 115 to 300 GeV. Model independent upper limits are given for the product of the cross section and branching fraction for gluon fusion and b quark associated production. They are the most stringent limits obtained to date in this channel.

Search for neutral MSSM Higgs bosons decaying to $\mu^{+} \mu^{-}$ in pp collisions at $ \sqrt{s} =$ 7 and 8 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. Results are reported on a search for decays of a pseudoscalar A boson into a Z boson and a light scalar h boson, where the Z boson decays into a pair of oppositely-charged electrons or muons, and the h boson decays into b anti-b. The search is based on data from proton-proton collisions at a center-of-mass energy sqrt(s)=8 TeV collected with the CMS detector, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The h boson is assumed to be the recently discovered standard model-like Higgs boson with a mass of 125 GeV. With no evidence for signal, upper limits are obtained on the product of the production cross section and the branching fraction of the A boson in the Zh channel. Results are also interpreted in the context of two Higgs doublet models.

Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in llbb final states;CMS Collaboration;2016;HEPData


Abstract: A search for neutral Higgs bosons in the minimal supersymmetric extension of the standard model (MSSM) decaying to tau-lepton pairs in pp collisions is performed, using events recorded by the CMS experiment at the LHC. The dataset corresponds to an integrated luminosity of 24.6 fb$^{-1}$, with 4.9 fb$^{-1}$ at 7 TeV and 19.7 fb$^{-1}$ at 8 TeV. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes the case where the Higgs boson is produced in association with a b-quark jet. No excess is observed in the tau-lepton-pair invariant mass spectrum. Exclusion limits are presented in the MSSM parameter space for different benchmark scenarios, $m_\mathrm{h}^\text{max}$, $m_\mathrm{h}^{\text{mod}+}$, $m_\mathrm{h}^{\text{mod}-}$, light-stop, light-stau, $\tau$-phobic, and low-$m_\mathrm{H}$. Upper limits on the cross section times branching fraction for gluon fusion and b-quark associated Higgs boson production are also given.

Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. A search for a heavy Higgs boson in the $\mathrm{H \to WW}$ and $\mathrm{H \to ZZ}$ decay channels is reported. The search is based upon proton-proton collision data samples corresponding to an integrated luminosity of up to 5.1 fb$^{-1}$ at $\sqrt{s}$ = 7 TeV and up to 19.7 fb$^{-1}$ at $\sqrt{s}$ = 8 TeV, recorded by the CMS experiment at the CERN LHC. Several final states of the $\mathrm{H \to WW}$ and $\mathrm{H \to ZZ}$ decays are analyzed. The combined upper limit at the 95% confidence level on the product of the cross section and branching fraction exclude a Higgs boson with standard model-like couplings and decays in the $m_{\mathrm{H}}$ range from 145 to 1000 GeV. We also interpret the results in the context of an electroweak singlet extension of the standard model.

Search for a Higgs boson in the mass range from 145 to 1000 GeV decaying to a pair of W or Z bosons;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. The centrality dependence of the charged-particle pseudorapidity density measured with ALICE in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ over a broad pseudorapidity range is presented. This Letter extends the previous results reported by ALICE to more peripheral collisions. The broad pseudorapidity range allows precise estimates of the total number of produced charged particles.

Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03<$y_{\rm cms}$<3.53), mid (-1.37<$y_{\rm cms}$<0.43) and backward (-4.46<$y_{\rm cms}$<-2.96) centre of mass rapidities.

Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Hypertriton and anti-hypertriton measurement in Pb--Pb collisions. Lifetime determination, transverse momentum spectra, yields and coalescence parameter were measured and compared to other identified species.

$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. The pseudorapidity ($\eta$) and transverse-momentum ($p_{\rm T}$) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy $\sqrt{s}$ = 13 TeV. The pseudorapidity distribution in $|\eta|<$ 1.8 is reported for inelastic events and for events with at least one charged particle in $|\eta|<$ 1. The pseudorapidity density of charged particles produced in the pseudorapidity region $|\eta|<$ 0.5 is 5.31 $\pm$ 0.18 and 6.46 $\pm$ 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 $<$ $p_{\rm T}$ $<$ 20 GeV/c and $|\eta|<$ 0.8 for events with at least one charged particle in $|\eta|<$ 1 (INEL>0). The correlation between transverse momentum and particle multiplicity is also investigated by studying the evolution of the spectra with event multiplicity.

Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV;ALICE Collaboration;2016;HEPData


Abstract:
Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.

Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV;CMS Collaboration;2016;HEPData


Abstract: Jet multiplicity distributions in top quark pair (ttbar) events are measured in pp collisions at a centre-of-mass energy of 8 TeV with the CMS detector at the LHC using a data set corresponding to an integrated luminosity of 19.7 inverse-femtobarns. The measurement is performed in the dilepton decay channels (e+ e-, mu+ mu-, and e+/- mu-/+). The absolute and normalized differential cross sections for t-tbar production are measured as a function of the jet multiplicity in the event for different jet transverse momentum thresholds and the kinematic properties of the leading additional jets. The differential t-tbar-b and t-tbar-b-bbar cross sections are presented for the first time as a function of the kinematic properties of the leading additional b jets. Furthermore, the fraction of events without additional jets above a threshold is measured as a function of the transverse momenta of the leading additional jets and the scalar sum of the transverse momenta of all additional jets. The data are compared and found to be consistent with predictions from several perturbative quantum chromodynamics event generators and a next-to-leading order calculation.

Measurement of t-tbar production with additional jet activity, including b quark jets, in the dilepton channel using pp collisions at sqrt(s) = 8TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. Transverse momentum ($p_{\rm{T}}$) spectra of pions, kaons, and protons up to $p_{\rm{T}} = 20$ GeV/$c$ have been measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV using the ALICE detector for six different centrality classes covering 0-80%. The proton-to-pion and the kaon-to-pion ratios both show a distinct peak at $p_{\rm{T}} \approx 3$ GeV/$c$ in central Pb-Pb collisions that decreases towards more peripheral collisions. For $p_{\rm{T}} > 10$ GeV/$c$, the nuclear modification factor is found to be the same for all three particle species in each centrality interval within systematic uncertainties of 10-20%.

Centrality dependence of the nuclear modification factor of charged pions, kaons, and protons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV;ALICE Collaboration;2016;HEPData


Abstract:
The charge asymmetry in $\mathrm{t\bar{t}}$ events is measured using dilepton final states produced in pp collisions at the LHC at $\sqrt{s}=8\:$TeV. The data sample, collected with the CMS detector, corresponds to an integrated luminosity of 19.5 inverse femtobarns. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The charge asymmetry is measured from differences in kinematic distributions, unfolded to the parton level, of positively and negatively charged top quarks and leptons. The $\mathrm{t\bar{t}}$ and leptonic charge asymmetries are found to be 0.011 +/- 0.011 (stat) +/- 0.007 (syst) and 0.003 +/- 0.006 (stat) +/- 0.003 (syst), respectively. These results, as well as charge asymmetry measurements made as a function of $\mathrm{t\bar{t}}$ system kinematic properties, are in agreement with predictions of the standard model.

For the normalized differential cross sections as a function of $\Delta|y_\mathrm{t}|$ and $\Delta|\eta_{\ell}|$ the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the $\mathrm{t\bar{t}}$ system variables and $\Delta|y_\mathrm{t}|$ or $\Delta|\eta_{\ell}|$, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

The lower and upper $\Delta|y_\mathrm{t}|$ and $\Delta|\eta_{\ell}|$ bins (starting and ending at -2 and +2, respectively) contain underflow and overflow events, i.e. the complete distribution from -infinity to +infinity is covered.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.

Measurements of t t-bar charge asymmetry using dilepton final states in pp collisions at sqrt(s) = 8 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. The production of electrons from heavy-flavour hadron decays was measured as a function of transverse momentum ($p_{\rm T}$) in minimum-bias p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV with ALICE at the LHC. The measurement covers the $p_{\rm T}$ interval $0.5

Measurement of electrons from heavy-flavour hadron decays in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. A new set of measurements of the top quark mass are presented, based on the proton-proton data recorded by the CMS experiment at the LHC at sqrt(s) = 8 TeV corresponding to a luminosity of 19.7 inverse femtobarns. The top quark mass is measured using the lepton+jets, all-jets and dilepton decay channels, giving values of 172.35 +/- 0.16 (stat) +/- 0.48 (syst) GeV, 172.32 +/- 0.25 (stat) +/- 0.59 (syst) GeV, and 172.82 +/- 0.19 (stat) +/- 1.22 (syst) GeV, respectively. When combined with the published CMS results at sqrt(s) = 7 TeV, they provide a top quark mass measurement of 172.44+/- 0.13 (stat) +/- 0.47 (syst) GeV. The top quark mass is also studied as a function of the event kinematical properties in the lepton+jets decay channel. No indications of a kinematic bias are observed and the collision data are consistent with a range of predictions from current theoretical models of ttbar production.

Measurement of the top quark mass using proton-proton data at ${\sqrt{(s)}}$ = 7 and 8 TeV;CMS Collaboration;2016;HEPData


Abstract: Fermilab-Tevatron. Measurement of the ratios of cross section for B-JET to JET production in association with a Z0 boson in antiproton-proton interactions at a centre of mass energy of 1.96 TeV. The data, with an integrated luminosity of 9.7 fb-1, is presented as functions of the jet and Z0 transverse momentum, the jet pseudorapidity and the azimuthal angle between the Z0 and the closest jet. Events must have at least one jet with jets being reconstructed from energy deposits in the calorimeter using an iterative mid-point cone algorithm with delta R = 0.5. Events are rejected if the missing ET is > 60 GeV to reduce t-tbar contamination.

Measurement of the ratio of differential cross sections {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet) in ppbar collisions at sqrt(s)=1.96 TeV;D0 Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurements of charged pion, kaon and (anti)proton production at mid-rapidity in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV recorded in the autumn of 2010 as a function of centrality. The measurements cover the transverse momentum (pT) range from 100 MeV to 3 GeV for pions, 200 MeV to 3 GeV for kaons, and 300 MeV to 4.6 GeV for (anti)protons. These data extend previous measurements for the most central bin (centrality of 0-5%) available from http://hepdata.cedar.ac.uk/view/ins1126966.

Centrality dependence of Pi, K, p production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV;ALICE Collaboration;2018;HEPData


Abstract:
CERN-LHC. The ALICE measurement of K$^0_{\rm S}$ and $\rm\Lambda$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV is presented. The transverse momentum ($p_{\rm T}$) spectra are shown for several collision centrality intervals and in the $p_{\rm T}$ range from 0.4 GeV/$c$ (0.6 GeV/$c$ for $\rm\Lambda$) to 12 GeV/$c$. The $p_{\rm T}$ dependence of the $\rm \Lambda$/K$^0_{\rm S}$ ratios exhibits maxima in the vicinity of 3 GeV/$c$, and the positions of the maxima shift towards higher $p_{\rm T}$ with increasing collision centrality. The magnitude of these maxima increases by almost a factor of three between most peripheral and most central Pb-Pb collisions. This baryon excess at intermediate $p_{\rm T}$ is not observed in pp interactions at sqrt(s) = 0.9 TeV and at sqrt(s) = 7 TeV. Qualitatively, the baryon enhancement in heavy-ion collisions is expected from radial flow. However, the measured $p_{\rm T}$ spectra above 2 GeV/$c$ progressively decouple from hydrodynamical-model calculations. For higher values of $p_{\rm T}$, models that incorporate the influence of the medium on the fragmentation and hadronization processes describe qualitatively the $p_{\rm T}$ dependence of the $\rm\Lambda$/K$^0_{\rm S}$ ratio
Note:(Update APR 2016) total integrated mid-rapidity yields for Lambda and K0s added.

K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. The ratio of the production cross sections times branching fractions $\sigma(B_c^{\pm})B(B_c^{\pm} \to J/\psi \pi^{\pm}) /((\sigma(B^{\pm}) B(B^{\pm} \to J/\psi K^{\pm}))$ is studied in proton-proton collisions at a center-of-mass energy of 7 TeV with the CMS detector at the LHC. The kinematic region investigated requires $B_c^{\pm}$ and $B^{\pm}$ mesons with transverse momentum $p_T$ > 15 GeV and rapidity |y| < 1.6. The data sample corresponds to an integrated luminosity of 5.1 fb$^{-1}$. The ratio is determined to be [0.48 $\pm$ 0.05(stat) $\pm$ 0.03(syst) $\pm$ 0.05 ($\tau_{Bc})$]% . The $B_c^{\pm} \to J/\psi \pi^{\pm} \pi^{\pm} \pi^{\mp}$ is also observed in the same data sample. Using a model-independent method developed to measure the efficiency given the presence of resonant behaviour in the three-pion system, the ratio of the branching fractions $B(B_c^{\pm} \to J/\psi \pi^{\pm} \pi^{\pm} \pi^{\mp})/B(B_c^{\pm} \to J/\psi \pi^{\pm})$ is measured to be 2.55 $\pm$ 0.80(stat) $\pm$ 0.33(syst) $\mathrm{^{+ 0.04}_{-0.01} }(\tau_{Bc}$), consistent with the previous LHCb result.

Measurement of the ratio B(Bc+/- to J/psi pi+/- pi+/- pi-/+)/B(Bc+/- to J/psi pi+/-) and the production cross sections times branching fractions of Bc+/- to J/psi pi+/- and B+/- to J/psi K+/- in pp collisions at sqrt(s) = 7 TeV;CMS Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurements of the PT distributions of primary charged particles produced in non-single-diffractive (NSD) proton-Lead collisions at a centre-of-mass energy/nucleon of 5.02 TeV. The data, collected during the September 2012 LHC run, cover the PT region 0.5 to 20 GeV/c in 3 near central rapidity regions, |eta|<0.3, 0.3-0.8 and 0.8-1.3. The nuclear modification factor R_pPb is determined to be consistent with unity above a PT of 2 GeV.

Transverse Momentum Distribution and Nuclear Modification Factor of Charged Particles in p-Pb Collisions at sqrt{s_NN} = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: A first measurement of the top quark spin asymmetry, sensitive to the top quark polarisation, in t-channel single top quark production is presented. It is based on a sample of pp collisions at a centre-of-mass energy of 8 TeV corresponding to an integrated luminosity of 19.7 inverse-femtobarns. A high-purity sample of t-channel single top quark events with an isolated muon is selected. Signal and background components are estimated using a fit to data. A differential cross section measurement, corrected for detector effects, of an angular observable sensitive to the top quark polarisation is performed. The differential distribution is used to extract a top quark spin asymmetry of 0.26 +/- 0.03 (stat) +/- 0.10 (syst), which is compatible with a p-value of 4.6% with the standard model prediction of 0.44.

Measurement of Top Quark Polarisation in T-Channel Single Top Quark Production;CMS Collaboration;2016;HEPData


Abstract:
CERN-LHC. The angular distributions and the differential branching fraction of the decay ${\rm B}^0 \to {\rm K^*(892)}^0 \mu^+ \mu^-$ are studied using data corresponding to an integrated luminosity of 20.5 fb$^{-1}$ collected with the CMS detector at the LHC in pp collisions at $\sqrt{s} = 8$ TeV. From 1430 signal decays, the forward-backward asymmetry of the muons, the ${\rm K^*(892)}^0$ longitudinal polarization fraction, and the differential branching fraction are determined as a function of the dimuon invariant mass squared.

UPDATE (16 MAY 2017): changed 0.64 to 0.63 for FL in first bin of Table 2 on request of Mauro Dinardo (CMS).

Angular analysis of the decay B0 to K*0 mu mu from pp collisions at sqrt(s) = 8 TeV;CMS Collaboration;2017;HEPData


Abstract: CERN-LHC. The ALICE collaboration reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons at central rapidity in the transverse momentum $p_{\rm T}$ interval 1-10 GeV/$c$, in pp collisions at $\sqrt{s}$ = 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. The integrated visible cross section was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total beauty production cross section.

Beauty production in pp collisions at $\sqrt{s}$ = 2.76 TeV measured via semi-electronic decays;ALICE Collaboration;2022;HEPData


MATLAS dwarfs structure and morphology

VizieR online Data Catalogue associated with article published in journal Monthly Notices of the Royal Astronomical Society with title ' Structure and morphology of the MATLAS dwarf galaxies and their central nuclei.' (bibcode: 2021MNRAS.506.5494P)

MATLAS dwarfs structure and morphology;M. Poulain;2021;Centre de Donnees Strasbourg (CDS)


Abstract: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.

CCDC 2385973: Experimental Crystal Structure Determination;Şahin, Neslihan;2024;Cambridge Crystallographic Data Centre

Related Article: Neslihan Şahin,  İsmail Özdemir,  David Sémeril|2024|Molbank|2024|M1911|doi:10.3390/M1911


CCDC 2385094: Experimental Crystal Structure Determination;Şahin, Neslihan;2024;Cambridge Crystallographic Data Centre

Related Article: Neslihan Şahin,  İsmail Özdemir,  David Sémeril|2024|Molbank|2024|M1913|doi:10.3390/M1913


CCDC 2340227: Experimental Crystal Structure Determination;Li, Shengxu;2024;Cambridge Crystallographic Data Centre

Related Article: Shengxu Li|2024|CSD Communication||| Related Article: Shengxu Li, Shunqi Xu, En Lin, Tonghai Wang, Haoyong Yang, Junyi Han, Yuxiang Zhao, Qunji Xue, Paolo Samorì, Zhenjie Zhang, Tao Zhang |2025|Nature Chemistry|17|226|doi:10.1038/s41557-024-01690-y


CCDC 2359207: Experimental Crystal Structure Determination;Ng, Shawn;2024;Cambridge Crystallographic Data Centre

Related Article: Shawn Ng, Casey Howshall, Thanh Nhat Ho, Binh Khanh Mai, Yuebiao Zhou, Can Qin, Kai Ze Tee, Peng Liu, Filippo Romiti, Amir H. Hoveyda|2024|Science|386|167|doi:10.1126/science.adr8612


CCDC 2367224: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre

Related Article: Lucas Popek, Gauthier Lefebvre, Vincent Debrauwer, David Roubaud, Nicolas Blanchard, Christophe Meyer, Vincent Bizet|2024|Org.Lett.|26|10369|doi:10.1021/acs.orglett.4c03972


9-methylindolizino[3,2,1-kl]acridin-5-ium-13b(9H)-yl radical hexafluorophosphate acetonitrile solvate

CCDC 2367356: Experimental Crystal Structure Determination;de Rouville, Henri-Pierre Jacquot;2024;Cambridge Crystallographic Data Centre

Related Article: Henri-Pierre Jacquot de Rouville, Christophe Gourlaouen, David Bardelang, Nolwenn Le Breton, Jas S. Ward, Laurent Ruhlmann, Jean-Marc Vincent, Damien Jardel, Kari Rissanen, Jean-Louis Clément, Sylvie Choua, Valérie Heitz|2024|J.Am.Chem.Soc.|147|1823|doi:10.1021/jacs.4c13807


CCDC 2370315: Experimental Crystal Structure Determination;KILIÇ, HURİYE AKDAŞ;2024;Cambridge Crystallographic Data Centre

Related Article: HURİYE AKDAŞ KILIÇ, ERNEST GRAF, MİR WAİS HOSSEİNİ, NATHALİE KYRİTSAKAS|2022|Turk.J.Chem.|46|1541|doi:10.55730/1300-0527.3459


silver hexafluoroantimonate 5,11,17,23-tetra-t-butyl-25,26,27,28-tetrakis(3-(methylsulfanyl)propoxy)-2,8,14,20-tetrathiacalix[4]arene 1,4-dioxane methanol solvate

CCDC 2370316: Experimental Crystal Structure Determination;KILIÇ, HURİYE AKDAŞ;2024;Cambridge Crystallographic Data Centre


CCDC 2340230: Experimental Crystal Structure Determination;Li, Shengxu;2024;Cambridge Crystallographic Data Centre


CCDC 2370333: Experimental Crystal Structure Determination;Li, Shengxu;2024;Cambridge Crystallographic Data Centre


CCDC 2372000: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2372001: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2372002: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2372003: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2375271: Experimental Crystal Structure Determination;Al-Handawi, Marieh B.;2024;Cambridge Crystallographic Data Centre

Related Article: Marieh B. Al-Handawi, Patrick Commins, Ahmed S. Dalaq, Pedro A. Santos-Florez, Srujana Polavaram, Pascal Didier, Durga Prasad Karothu, Qiang Zhu, Mohammed Daqaq, Liang Li, Panče Naumov |2024|Nat.Commun.|15|8095|doi:10.1038/s41467-024-51625-x


CCDC 2342756: Experimental Crystal Structure Determination;Gao, Yan-Li;2024;Cambridge Crystallographic Data Centre

Related Article: Yan-Li Gao, Li Li, Katsuya Inoue, Mohamedally Kurmoo|2024|Inorg.Chem.|63|22328|doi:10.1021/acs.inorgchem.4c02218 Related Article: Yan-Li Gao, Li Li, Katsuya Inoue, Mohamedally Kurmoo|2024|Inorg.Chem.|63|22328|doi:10.1021/acs.inorgchem.4c02218


CCDC 2342757: Experimental Crystal Structure Determination;Gao, Yan-Li;2024;Cambridge Crystallographic Data Centre


CCDC 2342758: Experimental Crystal Structure Determination;Gao, Yan-Li;2024;Cambridge Crystallographic Data Centre


CCDC 2342759: Experimental Crystal Structure Determination;Gao, Yan-Li;2024;Cambridge Crystallographic Data Centre


(5,8-dioxa-2,11-diazadodeca-1,11-diene-1,12-diyl)bis[(pyridine-6,2-diyl)methylene] bis(4-methoxybenzoate)-copper(i) tetrafluoroborate acetonitrile solvate

CCDC 2300384: Experimental Crystal Structure Determination;del Giudice, Nicolas;2024;Cambridge Crystallographic Data Centre

Related Article: Nicolas del Giudice, Guillaume Voegeli, Jean-Marc Strub, Benoît Heinrich, Laurent Douce|2024|Inorg.Chem.|63|6103|doi:10.1021/acs.inorgchem.4c00728


CCDC 2329904: Experimental Crystal Structure Determination;Rognan, Charlou;2024;Cambridge Crystallographic Data Centre

Related Article: Charlou Rognan, Pierre Locquet, Romain Pertschi, Nicolas Girard, Mihaela Gulea|2024|Adv.Synth.Catal.|366|4078|doi:10.1002/adsc.202400714


CCDC 2329905: Experimental Crystal Structure Determination;Rognan, Charlou;2024;Cambridge Crystallographic Data Centre


decakis(mu-hydroxo)-octakis(mu-benzoylacetonato)-octakis(benzoylacetonato)-nona-ytterbium(iii) chloride ethanol solvate

CCDC 2016566: Experimental Crystal Structure Determination;Panguluri, Sai P. K.;2024;Cambridge Crystallographic Data Centre

Related Article: Sai P. K. Panguluri, Elsa Jourdain, Papri Chakraborty, Svetlana Klyatskaya, Manfred M. Kappes, Aline M. Nonat, Loïc J. Charbonnière, Mario Ruben|2024|J.Am.Chem.Soc.|146|13083|doi:10.1021/jacs.3c14527


decakis(mu-hydroxo)-octakis(mu-benzoylacetonato)-octakis(benzoylacetonato)-nona-gadolinium(iii) chloride ethanol solvate

CCDC 2016567: Experimental Crystal Structure Determination;Panguluri, Sai P. K.;2024;Cambridge Crystallographic Data Centre


decakis(mu-hydroxo)-octakis(mu-benzoylacetonato)-octakis(benzoylacetonato)-nona-terbium(iii) chloride ethanol solvate

CCDC 2017536: Experimental Crystal Structure Determination;Panguluri, Sai P. K.;2024;Cambridge Crystallographic Data Centre


decakis(mu-hydroxo)-octakis(mu-benzoylacetonato)-octakis(benzoylacetonato)-nona-holmium(iii) chloride ethanol solvate

CCDC 2331085: Experimental Crystal Structure Determination;Panguluri, Sai P. K.;2024;Cambridge Crystallographic Data Centre


CCDC 2302867: Experimental Crystal Structure Determination;Casas, Jaison;2024;Cambridge Crystallographic Data Centre

Related Article: Jaison Casas, David Pianca, Nolwenn Le Breton, Abdelaziz Jouaiti, Christophe Gourlaouen, Marine Desage-El Murr, Steven Le Vot, Sylvie Choua, Sylvie Ferlay|2024|Inorg.Chem.|63|4802|doi:10.1021/acs.inorgchem.3c04550


hexakis(mu-benzoato)-(mu-oxido)-tris(pyridine)-tri-gallium perchlorate pyridine solvate

CCDC 2334338: Experimental Crystal Structure Determination;le Mardelé, Florian;2024;Cambridge Crystallographic Data Centre

Related Article: Florian le Mardelé, Ivan Mohelský, Jan Wyzula, Milan Orlita, Philippe Turek, Filippo Troiani, Athanassios K. Boudalis|2024|arXiv.org, condensed matter|||doi:10.48550/arXiv.2403.11214 Related Article: Florian le Mardelé,  Ivan Mohelský,  Jan Wyzula,  Milan Orlita,  Philippe Turek,  Filippo Troiani,  Athanassios K. Boudalis|2025|Nat.Commun.|16|1198|doi:10.1038/s41467-025-56453-1


CCDC 2302868: Experimental Crystal Structure Determination;Casas, Jaison;2024;Cambridge Crystallographic Data Centre


CCDC 2338036: Experimental Crystal Structure Determination;Israfilov, Nizami;2024;Cambridge Crystallographic Data Centre

Related Article: Nizami Israfilov, Leo Meyer, Shabnam Feyziyeva, Nathalie Kyritsakas-Gruber, Benoit Louis, Jean-Marc Planeix|2024|J.Solid State Chem.|332|124582|doi:10.1016/j.jssc.2024.124582


CCDC 2338499: Experimental Crystal Structure Determination;Ballerini, Lavinia;2024;Cambridge Crystallographic Data Centre

Related Article: Lavinia Ballerini, Wei-Min Zhang, Thomaz Groizard, Christophe Gourlaouen, Federico Polo, Abdelaziz Jouaiti, Hai-Ching Su, Matteo Mauro |2024|J.Mater.Chem.C|12|12769|doi:10.1039/d4tc02040e


CCDC 2338500: Experimental Crystal Structure Determination;Ballerini, Lavinia;2024;Cambridge Crystallographic Data Centre


CCDC 2338501: Experimental Crystal Structure Determination;Ballerini, Lavinia;2024;Cambridge Crystallographic Data Centre


CCDC 2338502: Experimental Crystal Structure Determination;Ballerini, Lavinia;2024;Cambridge Crystallographic Data Centre


Abstract: An entry from the Inorganic Crystal Structure Database, the world’s repository for inorganic crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the joint CCDC and FIZ Karlsruhe Access Structures service and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.

Inorganic Crystal Structure Database (ICSD)

CSD 2338838: Experimental Crystal Structure Determination;Örs, Taylan;2024;FIZ Karlsruhe - Leibniz Institute for Information Infrastructure

Related Article: Taylan Örs, Irena Deroche, Corentin Chatelard, Mathias Dodin, Raquel Martinez-Franco, Alain Tuel, Jean-Louis Paillaud|2024|Symmetry|16|477|doi:10.3390/sym16040477


Related Article: Rong-Ran Liang, Shunqi Xu, Zongsu Han, Yihao Yang, Kun-Yu Wang, Zhehao Huang, Joshua Rushlow, Peiyu Cai, Paolo SamorA A{not}, Hong-Cai Zhou|2024|J.Am.Chem.Soc.|146|9811|doi:10.1021/jacs.3c14487 Related Article: Rong-Ran Liang, Shunqi Xu, Zongsu Han, Yihao Yang, Kun-Yu Wang, Zhehao Huang, Joshua Rushlow, Peiyu Cai, Paolo Samorì, Hong-Cai Zhou|2024|J.Am.Chem.Soc.|146|9811|doi:10.1021/jacs.3c14487

CCDC 2304331: Experimental Crystal Structure Determination;Liang, Rong-Ran;2024;Cambridge Crystallographic Data Centre


(mu-cycloheptatriene trianion)-tris(borohydride)-tris(tetrahydrofuran)-di-erbium(iii) tetrahydrofuran solvate

Related Article: Adrian Hauser, Luca Münzfeld, Sören Schlittenhardt, Cedric Uhlmann, Louis Leyen, Eufemio Moreno-Pineda, Mario Ruben, Peter W. Roesky|2024|J.Am.Chem.Soc.|146|13760|doi:10.1021/jacs.3c12214

CCDC 2303890: Experimental Crystal Structure Determination;Hauser, Adrian;2024;Cambridge Crystallographic Data Centre


Related Article: Sotaro Kusumoto, Kaede Wakabayashi, Kenta Rakumitsu, Jack Harrowfield, Yang Kim, Yoshihiro Koide|2024|Chem.-Eur.J.|30|e202401564|doi:10.1002/chem.202401564

CCDC 2345616: Experimental Crystal Structure Determination;Kusumoto, Sotaro;2024;Cambridge Crystallographic Data Centre


4,4',4'',4'''-(cyclobutane-1,2,3,4-tetrayl)tetra(pyridin-1-ium) oxonium pentanitrate dihydrate

CCDC 2345617: Experimental Crystal Structure Determination;Kusumoto, Sotaro;2024;Cambridge Crystallographic Data Centre


Related Article: António G. Costa,  Gonçalo Lopes,  João F. G. Rodrigues,  Isabel C. Santos,  Dulce Simão,  Elsa B. Lopes,  Laura C. J. Pereira,  Nolwenn Le Breton,  Sylvie Choua,  Stéphane A. Baudron,  Manuel Almeida,  Sandra Rabaça|2024|Crystals|14|469|doi:10.3390/cryst14050469

CCDC 2346079: Experimental Crystal Structure Determination;Costa, António G.;2024;Cambridge Crystallographic Data Centre


CCDC 2346080: Experimental Crystal Structure Determination;Costa, António G.;2024;Cambridge Crystallographic Data Centre


CCDC 2346081: Experimental Crystal Structure Determination;Costa, António G.;2024;Cambridge Crystallographic Data Centre


Related Article: Tuan-Anh Phan, Matthieu Jouffroy, Dominique Matt, Nicola Armaroli, Alejandra Saavedra Moncada, Elisa Bandini, Béatrice Delavaux-Nicot, Jean-François Nierengarten, Dominique Armspach|2024|Chem.-Eur.J.|30|e202302750|doi:10.1002/chem.202302750

CCDC 2280885: Experimental Crystal Structure Determination;Phan, Tuan-Anh;2024;Cambridge Crystallographic Data Centre


CCDC 2280887: Experimental Crystal Structure Determination;Phan, Tuan-Anh;2024;Cambridge Crystallographic Data Centre


CCDC 2280888: Experimental Crystal Structure Determination;Phan, Tuan-Anh;2024;Cambridge Crystallographic Data Centre


Related Article: Johnny Hu, Jean-Pierre Launay, Alain Chaumont, Valérie Heitz, Henri-Pierre Jacquot de Rouville|2024|Chem.-Eur.J.|30|e202401866|doi:10.1002/chem.202401866

CCDC 2290247: Experimental Crystal Structure Determination;Hu, Johnny;2024;Cambridge Crystallographic Data Centre


9,9'-[pyridin-1-ium-2,6-diylbis(5-methoxy-3,1-phenylene)]bis(acridin-10-ium) tris(hydrogen sulfate) methanol solvate sesquihydrate

CCDC 2290248: Experimental Crystal Structure Determination;Hu, Johnny;2024;Cambridge Crystallographic Data Centre


9,9'-[pyridine-2,6-diylbis(3,1-phenylene)]bis(acridin-10-ium) bis(chloride) unknown solvate

CCDC 2290249: Experimental Crystal Structure Determination;Hu, Johnny;2024;Cambridge Crystallographic Data Centre


Related Article: Josef Taut, Frederik Schleife, Martin Börner, Clément Bonnot, Henri-Pierre Jacquot de Rouville, Jean-Claude Chambron, Berthold Kersting|2024|Eur.J.Inorg.Chem.|27|e202300580|doi:10.1002/ejic.202300580

CCDC 2295823: Experimental Crystal Structure Determination;Taut, Josef;2024;Cambridge Crystallographic Data Centre


CCDC 2295824: Experimental Crystal Structure Determination;Taut, Josef;2024;Cambridge Crystallographic Data Centre


CCDC 2295825: Experimental Crystal Structure Determination;Taut, Josef;2024;Cambridge Crystallographic Data Centre


Related Article: Morgane Mando, Fabienne Grellepois, Aurélien Blanc, Eric Hénon, Emmanuel Riguet|2024|Chem.-Eur.J.|30|e202304138|doi:10.1002/chem.202304138

CCDC 2298733: Experimental Crystal Structure Determination;Mando, Morgane;2024;Cambridge Crystallographic Data Centre


CCDC 2298735: Experimental Crystal Structure Determination;Mando, Morgane;2024;Cambridge Crystallographic Data Centre


CCDC 2298740: Experimental Crystal Structure Determination;Mando, Morgane;2024;Cambridge Crystallographic Data Centre


CCDC 2298741: Experimental Crystal Structure Determination;Mando, Morgane;2024;Cambridge Crystallographic Data Centre


CCDC 2300383: Experimental Crystal Structure Determination;del Giudice, Nicolas;2024;Cambridge Crystallographic Data Centre


(5,8-dioxa-2,11-diazadodeca-1,11-diene-1,12-diyl)bis[(pyridine-6,2-diyl)methylene] bis(4-methoxybenzoate)-copper(i) perchlorate dichloromethane solvate

CCDC 2300385: Experimental Crystal Structure Determination;del Giudice, Nicolas;2024;Cambridge Crystallographic Data Centre


Related Article: Lucas Popek, Murat Cihan, Nicolas Blanchard, Vincent Bizet|2024|Angew.Chem.,Int.Ed.|63||doi:10.1002/anie.202315909

CCDC 2302175: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2302176: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


CCDC 2302177: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


Related Article: Víctor Quezada,  Mariña Castroagudín,  Felipe Verdugo,  Sergio Ortiz,  Guillermo Zaragoza,  Fabiane M. Nachtigall,  Francisco A. A. Reis,  Alejandro Castro-Alvarez,  Leonardo S. Santos,  Ronald Nelson|2024|Molecules|29|1604|doi:10.3390/molecules29071604

CCDC 2302398: Experimental Crystal Structure Determination;Quezada, Víctor;2024;Cambridge Crystallographic Data Centre


Related Article: David Matchavariani, Lucas Popek, Jorge Juan Cabrera-Trujillo, Thi Mo Nguyen, Nicolas Blanchard, Karinne Miqueu, Dominique Cahard, Vincent Bizet|2024|Adv.Synth.Catal.|366|3481|doi:10.1002/adsc.202400446

CCDC 2303456: Experimental Crystal Structure Determination;Matchavariani, David;2024;Cambridge Crystallographic Data Centre


CCDC 2303457: Experimental Crystal Structure Determination;Matchavariani, David;2024;Cambridge Crystallographic Data Centre


CCDC 2303458: Experimental Crystal Structure Determination;Matchavariani, David;2024;Cambridge Crystallographic Data Centre


Related Article: Thi Mo Nguyen, Lucas Popek, David Matchavariani, Nicolas Blanchard, Vincent Bizet, Dominique Cahard|2024|Org.Lett.|26|365|doi:10.1021/acs.orglett.3c04043 Related Article: David Matchavariani, Lucas Popek, Jorge Juan Cabrera-Trujillo, Thi Mo Nguyen, Nicolas Blanchard, Karinne Miqueu, Dominique Cahard, Vincent Bizet|2024|Adv.Synth.Catal.|366|3481|doi:10.1002/adsc.202400446

CCDC 2303459: Experimental Crystal Structure Determination;Nguyen, Thi Mo;2024;Cambridge Crystallographic Data Centre


CCDC 2303460: Experimental Crystal Structure Determination;Nguyen, Thi Mo;2024;Cambridge Crystallographic Data Centre


CCDC 2303461: Experimental Crystal Structure Determination;Matchavariani, David;2024;Cambridge Crystallographic Data Centre


CCDC 2303462: Experimental Crystal Structure Determination;Matchavariani, David;2024;Cambridge Crystallographic Data Centre


(mu-cycloheptatriene trianion)-tris(borohydride)-tris(tetrahydrofuran)-di-yttrium(iii) tetrahydrofuran solvate

CCDC 2303889: Experimental Crystal Structure Determination;Hauser, Adrian;2024;Cambridge Crystallographic Data Centre


CCDC 2303891: Experimental Crystal Structure Determination;Hauser, Adrian;2024;Cambridge Crystallographic Data Centre


CCDC 2303892: Experimental Crystal Structure Determination;Hauser, Adrian;2024;Cambridge Crystallographic Data Centre


CCDC 2303893: Experimental Crystal Structure Determination;Hauser, Adrian;2024;Cambridge Crystallographic Data Centre


CCDC 2304332: Experimental Crystal Structure Determination;Liang, Rong-Ran;2024;Cambridge Crystallographic Data Centre


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CCDC 2304515: Experimental Crystal Structure Determination;Cao, Chen;2024;Cambridge Crystallographic Data Centre


CCDC 2304516: Experimental Crystal Structure Determination;Cao, Chen;2024;Cambridge Crystallographic Data Centre


CCDC 2304517: Experimental Crystal Structure Determination;Cao, Chen;2024;Cambridge Crystallographic Data Centre


CCDC 2304518: Experimental Crystal Structure Determination;Cao, Chen;2024;Cambridge Crystallographic Data Centre


CCDC 2304519: Experimental Crystal Structure Determination;Cao, Chen;2024;Cambridge Crystallographic Data Centre


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CCDC 2305608: Experimental Crystal Structure Determination;Ledneva, A. Yu.;2024;Cambridge Crystallographic Data Centre


CCDC 2305609: Experimental Crystal Structure Determination;Ledneva, A. Yu.;2024;Cambridge Crystallographic Data Centre


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CCDC 2271920: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


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CCDC 2309385: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309386: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309387: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309388: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309389: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309390: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309391: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309392: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


CCDC 2309393: Experimental Crystal Structure Determination;Uhlmann, Cedric;2024;Cambridge Crystallographic Data Centre


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CCDC 2309553: Experimental Crystal Structure Determination;Zhang, Kai-Li;2024;Cambridge Crystallographic Data Centre


CCDC 2309554: Experimental Crystal Structure Determination;Zhang, Kai-Li;2024;Cambridge Crystallographic Data Centre


CCDC 2309555: Experimental Crystal Structure Determination;Zhang, Kai-Li;2024;Cambridge Crystallographic Data Centre


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CCDC 2260556: Experimental Crystal Structure Determination;Stoerkler, Timothée;2024;Cambridge Crystallographic Data Centre


CCDC 2260557: Experimental Crystal Structure Determination;Stoerkler, Timothée;2024;Cambridge Crystallographic Data Centre


bis{2,2'-(pyridine-2,6-diyl)bis[6-(3,5-di-t-butylphenyl)imidazo[1,2-a]pyridine]}-zinc(ii) bis(tetrafluoroborate) acetone unknown solvate

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CCDC 2239324: Experimental Crystal Structure Determination;Giuso, Valerio;2023;Cambridge Crystallographic Data Centre


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CCDC 2261547: Experimental Crystal Structure Determination;Carvalho, Mary-Ambre;2023;Cambridge Crystallographic Data Centre


CCDC 2261554: Experimental Crystal Structure Determination;Carvalho, Mary-Ambre;2023;Cambridge Crystallographic Data Centre


CCDC 2261556: Experimental Crystal Structure Determination;Carvalho, Mary-Ambre;2023;Cambridge Crystallographic Data Centre


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CCDC 2262425: Experimental Crystal Structure Determination;Yahya, Mohamed;2024;Cambridge Crystallographic Data Centre


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CCDC 2263319: Experimental Crystal Structure Determination;Liu, Haijuan;2023;Cambridge Crystallographic Data Centre


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CCDC 2265379: Experimental Crystal Structure Determination;Brouillac, Clément;2024;Cambridge Crystallographic Data Centre


CCDC 2265380: Experimental Crystal Structure Determination;Brouillac, Clément;2024;Cambridge Crystallographic Data Centre


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CCDC 2269564: Experimental Crystal Structure Determination;Koutsopetras, Ilias;2023;Cambridge Crystallographic Data Centre


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CCDC 2270481: Experimental Crystal Structure Determination;Xu, Xuejuan;2023;Cambridge Crystallographic Data Centre


CCDC 2270482: Experimental Crystal Structure Determination;Xu, Xuejuan;2023;Cambridge Crystallographic Data Centre


CCDC 2270483: Experimental Crystal Structure Determination;Xu, Xuejuan;2023;Cambridge Crystallographic Data Centre


(1,3-bis[2,6-bis(diphenylmethyl)-4-methylphenyl]-1,3-dihydro-2H-imidazol-2-ylidene)-ethyl-zinc(ii) tetrakis(pentafluorophenyl)borate n-pentane unknown solvate

CCDC 2270484: Experimental Crystal Structure Determination;Xu, Xuejuan;2023;Cambridge Crystallographic Data Centre


CCDC 2270615: Experimental Crystal Structure Determination;Xu, Xuejuan;2023;Cambridge Crystallographic Data Centre


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CCDC 2271673: Experimental Crystal Structure Determination;Leblay, Rébecca;2024;Cambridge Crystallographic Data Centre


CCDC 2271674: Experimental Crystal Structure Determination;Leblay, Rébecca;2024;Cambridge Crystallographic Data Centre


CCDC 2271911: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271912: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271913: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271914: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271916: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271917: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271918: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271919: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271922: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271923: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271924: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271925: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271926: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


bis(3,5-di-t-butylphenyl)(methyl)telluronium trifluoromethanesulfonate cyclohexane solvate

CCDC 2271927: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


CCDC 2271928: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


bis[3,5-bis(trifluoromethyl)phenyl](methyl)telluronium chloride dichloromethane solvate

CCDC 2271929: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


bis[3,5-bis(trifluoromethyl)phenyl](methyl)telluronium tetrakis[3,5-bis(trifluoromethyl)phenyl]borate unknown solvate

CCDC 2271930: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


bis[3,5-bis(trifluoromethyl)phenyl](methyl)telluronium perchlorate dichloromethane solvate

CCDC 2271915: Experimental Crystal Structure Determination;Groslambert, Loïc;2023;Cambridge Crystallographic Data Centre


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CCDC 2276644: Experimental Crystal Structure Determination;Yu, Huajian;2023;Cambridge Crystallographic Data Centre


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CCDC 2280763: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


CCDC 2280764: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


bis((8-methyl-N-[(thiophen-2-yl)methyl]-3,6,10,13,16,19-hexaazabicyclo[6.6.6]icosan-1-aminium)-cobalt) chloride heptaperchlorate dimethyl sulfoxide solvate tetrahydrate

CCDC 2280765: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


CCDC 2280766: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


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CCDC 2280872: Experimental Crystal Structure Determination;Li, Jian;2023;Cambridge Crystallographic Data Centre


CCDC 2280873: Experimental Crystal Structure Determination;Li, Jian;2023;Cambridge Crystallographic Data Centre


CCDC 2280874: Experimental Crystal Structure Determination;Li, Jian;2023;Cambridge Crystallographic Data Centre


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CCDC 2281347: Experimental Crystal Structure Determination;Brach, Nicolas;2023;Cambridge Crystallographic Data Centre


CCDC 2281348: Experimental Crystal Structure Determination;Brach, Nicolas;2023;Cambridge Crystallographic Data Centre


CCDC 2281349: Experimental Crystal Structure Determination;Brach, Nicolas;2023;Cambridge Crystallographic Data Centre


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CCDC 2283039: Experimental Crystal Structure Determination;Thaggard, Grace C.;2023;Cambridge Crystallographic Data Centre


(15,35,135-trimethoxy-82,83,84,85,86,87,88,89-hexa-oxo-4,12,15-trioxa-1,3,13(1,2,4),6,10,17(1,4)-hexabenzena-8-dipyrrolo[3,4-e:3',4'-g]isoindolatricyclo[6.6.4.13,13]nonadecaphane cyclotriveratrylene hemicryptophane) dimethyl sulfoxide clathrate dimethyl sulfoxide solvate monohydrate

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CCDC 2283957: Experimental Crystal Structure Determination;Miton, Louise;2023;Cambridge Crystallographic Data Centre


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CCDC 2288023: Experimental Crystal Structure Determination;Panguluri, Sai P. K.;2024;Cambridge Crystallographic Data Centre


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CCDC 2233307: Experimental Crystal Structure Determination;Demangeat, Catherine;2023;Cambridge Crystallographic Data Centre


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CCDC 2236867: Experimental Crystal Structure Determination;Dake, Gaurav G.;2024;Cambridge Crystallographic Data Centre


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CCDC 2237343: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


catena-(bis(1-azoniabicyclo[2.2.2]octane) bis(mu-acetato)-bis(mu-(R,R)-tartrato)-octaoxo-tetra-uranium unknown solvate)

CCDC 2237344: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


catena-(tris(2,2'-bipyridine)-nickel bis(mu-oxalato)-bis(mu-(R,R)-tartrato)-octaoxo-tetra-uranium dimethylacetamide unknown solvate)

CCDC 2237345: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


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CCDC 2237593: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


CCDC 2237594: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


CCDC 2237595: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


CCDC 2237596: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


CCDC 2237597: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


CCDC 2237598: Experimental Crystal Structure Determination;Sokolov, Vladislav  A.;2024;Cambridge Crystallographic Data Centre


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CCDC 2238192: Experimental Crystal Structure Determination;Pakulski, Dawid;2023;Cambridge Crystallographic Data Centre


CCDC 2238193: Experimental Crystal Structure Determination;Pakulski, Dawid;2023;Cambridge Crystallographic Data Centre


lithium (hydrogen 9,13:26,22-bis(azeno)tetrabenzo[a,c,j,l][18]annulene) tetrabromo-iron dihydrate

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CCDC 2247606: Experimental Crystal Structure Determination;Torres‐Gutiérrez, Carolina;2023;Cambridge Crystallographic Data Centre


(6,6'-([1,1'-biphenyl]-2,2'-diyl)bis(2,2'-bipyridine))-chloro-iron(ii) hexafluorophosphate dichloromethane solvate

CCDC 2247607: Experimental Crystal Structure Determination;Torres‐Gutiérrez, Carolina;2023;Cambridge Crystallographic Data Centre


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CCDC 2251406: Experimental Crystal Structure Determination;Nguyen, Thi Mo;2024;Cambridge Crystallographic Data Centre


CCDC 2249876: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


CCDC 2249877: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


(2-[(8-amino-3,6,10,13,16,19-hexaazabicyclo[6.6.6]icosan-1-yl)carbamoyl]benzene-1-sulfonato)-magnesium chloride unknown solvate hexahydrate

CCDC 2249878: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


CCDC 2249879: Experimental Crystal Structure Determination;Donnelly, Paul S.;2023;Cambridge Crystallographic Data Centre


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CCDC 2254084: Experimental Crystal Structure Determination;Woods, Joseph F.;2023;Cambridge Crystallographic Data Centre


CCDC 2254085: Experimental Crystal Structure Determination;Woods, Joseph F.;2023;Cambridge Crystallographic Data Centre


CCDC 2254086: Experimental Crystal Structure Determination;Woods, Joseph F.;2023;Cambridge Crystallographic Data Centre


CCDC 2254105: Experimental Crystal Structure Determination;Woods, Joseph F.;2023;Cambridge Crystallographic Data Centre


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CCDC 2256019: Experimental Crystal Structure Determination;Munteanu, Tatiana;2023;Cambridge Crystallographic Data Centre


CCDC 2256023: Experimental Crystal Structure Determination;Munteanu, Tatiana;2023;Cambridge Crystallographic Data Centre


CCDC 2256032: Experimental Crystal Structure Determination;Munteanu, Tatiana;2023;Cambridge Crystallographic Data Centre


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CCDC 2204503: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


CCDC 2204504: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


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CSD 2204968: Experimental Crystal Structure Determination;Cornu;2022;FIZ Karlsruhe - Leibniz Institute for Information Infrastructure


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CCDC 2209948: Experimental Crystal Structure Determination;Vila, Jordi;2023;Cambridge Crystallographic Data Centre


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CCDC 2210775: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210776: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210777: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210778: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210779: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210780: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210781: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210782: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


CCDC 2210783: Experimental Crystal Structure Determination;Behzadi, Masoumeh;2023;Cambridge Crystallographic Data Centre


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CCDC 2212255: Experimental Crystal Structure Determination;Florent, Maxime;2024;Cambridge Crystallographic Data Centre


CCDC 2212256: Experimental Crystal Structure Determination;Florent, Maxime;2024;Cambridge Crystallographic Data Centre


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CCDC 2212564: Experimental Crystal Structure Determination;Feng, Zhao;2023;Cambridge Crystallographic Data Centre


CCDC 2213801: Experimental Crystal Structure Determination;Vila, Jordi;2023;Cambridge Crystallographic Data Centre


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CCDC 2204615: Experimental Crystal Structure Determination;Reiß, Andreas;2023;Cambridge Crystallographic Data Centre


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CCDC 2221093: Experimental Crystal Structure Determination;Popek, Lucas;2024;Cambridge Crystallographic Data Centre


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CCDC 2221949: Experimental Crystal Structure Determination;De Marco, Riccardo;2023;Cambridge Crystallographic Data Centre


CCDC 2221950: Experimental Crystal Structure Determination;De Marco, Riccardo;2023;Cambridge Crystallographic Data Centre


CCDC 2221951: Experimental Crystal Structure Determination;De Marco, Riccardo;2023;Cambridge Crystallographic Data Centre


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CCDC 2226772: Experimental Crystal Structure Determination;Appleton, Jordan L.;2023;Cambridge Crystallographic Data Centre


(2,9-bis(4-t-butyl-2,6-dimethylphenyl)-1,10-phenanthroline)-(2,9-dimethyl-1,10-phenanthroline)-copper hexafluorophosphate diethyl ether solvate

CCDC 2226783: Experimental Crystal Structure Determination;Appleton, Jordan L.;2023;Cambridge Crystallographic Data Centre


CCDC 2226784: Experimental Crystal Structure Determination;Appleton, Jordan L.;2023;Cambridge Crystallographic Data Centre


CCDC 2226785: Experimental Crystal Structure Determination;Appleton, Jordan L.;2023;Cambridge Crystallographic Data Centre


CCDC 2226786: Experimental Crystal Structure Determination;Appleton, Jordan L.;2023;Cambridge Crystallographic Data Centre


(1-{2-[(adamantan-1-yl)sulfanyl]ethyl}-3-methylimidazol-2-ylidene)-[cyclo-octa-1,5-diene]-rhodium hexafluorophosphate diethyl ether solvate

CCDC 2232591: Experimental Crystal Structure Determination;Vila, Jordi;2023;Cambridge Crystallographic Data Centre


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CCDC 2150133: Experimental Crystal Structure Determination;Filatov, Michael;2022;Cambridge Crystallographic Data Centre


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CCDC 2123376: Experimental Crystal Structure Determination;Schleife, Frederik;2022;Cambridge Crystallographic Data Centre


CCDC 2123377: Experimental Crystal Structure Determination;Schleife, Frederik;2022;Cambridge Crystallographic Data Centre


CCDC 2123378: Experimental Crystal Structure Determination;Schleife, Frederik;2022;Cambridge Crystallographic Data Centre


CCDC 2123379: Experimental Crystal Structure Determination;Schleife, Frederik;2022;Cambridge Crystallographic Data Centre


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CCDC 2161049: Experimental Crystal Structure Determination;Gebrezgiabher, Mamo;2022;Cambridge Crystallographic Data Centre


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CCDC 2168876: Experimental Crystal Structure Determination;Juarez‐Martinez, Yael;2022;Cambridge Crystallographic Data Centre


CCDC 2168877: Experimental Crystal Structure Determination;Juarez‐Martinez, Yael;2022;Cambridge Crystallographic Data Centre


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CCDC 2170911: Experimental Crystal Structure Determination;Elemo, Fikre;2023;Cambridge Crystallographic Data Centre


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CCDC 2177182: Experimental Crystal Structure Determination;Attias, Andre-Jean;2022;Cambridge Crystallographic Data Centre


CCDC 2177183: Experimental Crystal Structure Determination;Attias, Andre-Jean;2022;Cambridge Crystallographic Data Centre


CCDC 2177184: Experimental Crystal Structure Determination;Attias, Andre-Jean;2022;Cambridge Crystallographic Data Centre


CCDC 2177185: Experimental Crystal Structure Determination;Attias, Andre-Jean;2022;Cambridge Crystallographic Data Centre


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CCDC 2179315: Experimental Crystal Structure Determination;Marie, Hoffmann;2022;Cambridge Crystallographic Data Centre


CCDC 2179316: Experimental Crystal Structure Determination;Marie, Hoffmann;2022;Cambridge Crystallographic Data Centre


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CCDC 2184524: Experimental Crystal Structure Determination;Ajayi, Tolulope M.;2023;Cambridge Crystallographic Data Centre


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CCDC 2189743: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


catena-[tris(ethane-1,2-diamine)-cobalt (mu-pyrazine-2,3,5,6-tetracarboxylato)-dioxo-uranium nitrate monohydrate]

CCDC 2189744: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


CCDC 2189745: Experimental Crystal Structure Determination;Thuéry, Pierre;2023;Cambridge Crystallographic Data Centre


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CCDC 2192851: Experimental Crystal Structure Determination;Taran, Gheorghe;2023;Cambridge Crystallographic Data Centre


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CCDC 2112333: Experimental Crystal Structure Determination;Hkiri, Shaima;2022;Cambridge Crystallographic Data Centre


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CCDC 2115920: Experimental Crystal Structure Determination;Aubert, Emmanuel;2022;Cambridge Crystallographic Data Centre


CCDC 2115921: Experimental Crystal Structure Determination;Aubert, Emmanuel;2022;Cambridge Crystallographic Data Centre


CCDC 2115922: Experimental Crystal Structure Determination;Aubert, Emmanuel;2022;Cambridge Crystallographic Data Centre


CCDC 2115923: Experimental Crystal Structure Determination;Aubert, Emmanuel;2022;Cambridge Crystallographic Data Centre


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CCDC 2116366: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116367: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


(1,3-bis[2-(diphenylphosphanyl)phenyl]-2-ethyl-1,3-diazinan-2-yl)-nickel hexafluorophosphate tetrahydrofuran solvate

CCDC 2116368: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


bis((1,3-bis[2-(diphenylphosphanyl)phenyl]-1,3-diazinan-2-ylidene)-chloro-nickel) tetrachloro-nickel dichloromethane unknown solvate

CCDC 2116369: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116370: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116371: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116372: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116373: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


CCDC 2116374: Experimental Crystal Structure Determination;He, Fengkai;2022;Cambridge Crystallographic Data Centre


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CCDC 2124014: Experimental Crystal Structure Determination;Bizzarri, Claudia;2021;Cambridge Crystallographic Data Centre


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CCDC 2124212: Experimental Crystal Structure Determination;Hansjacob, Pierre;2023;Cambridge Crystallographic Data Centre


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CCDC 2009095: Experimental Crystal Structure Determination;Rosati, Marta;2022;Cambridge Crystallographic Data Centre


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CCDC 2103738: Experimental Crystal Structure Determination;Jouclas, Rémy;2024;Cambridge Crystallographic Data Centre


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CCDC 2036562: Experimental Crystal Structure Determination;Wang, Meng-Fan;2022;Cambridge Crystallographic Data Centre


CCDC 2036563: Experimental Crystal Structure Determination;Wang, Meng-Fan;2022;Cambridge Crystallographic Data Centre


CCDC 1889155: Experimental Crystal Structure Determination;Wang, Meng-Fan;2022;Cambridge Crystallographic Data Centre


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CCDC 2091982: Experimental Crystal Structure Determination;Wang, Zhi;2022;Cambridge Crystallographic Data Centre


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CCDC 2142803: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


CCDC 2142804: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


tetraethyl 2,2'-(naphtho[2,3-c][1,2,5]selenadiazole-4,9-diylidene)dipropanedioate n-hexane solvate

CCDC 2142805: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


CCDC 2142806: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


CCDC 2142807: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


CCDC 2142808: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


CCDC 2142809: Experimental Crystal Structure Determination;Ishigaki, Yusuke;2022;Cambridge Crystallographic Data Centre


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CCDC 2143452: Experimental Crystal Structure Determination;Shakouri, Shirin;2023;Cambridge Crystallographic Data Centre


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CCDC 2144457: Experimental Crystal Structure Determination;Weiss, Robin;2022;Cambridge Crystallographic Data Centre


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CCDC 2079088: Experimental Crystal Structure Determination;Knighton, Richard C.;2022;Cambridge Crystallographic Data Centre


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CCDC 2080821: Experimental Crystal Structure Determination;Devonport, Jack;2021;Cambridge Crystallographic Data Centre


CCDC 2080822: Experimental Crystal Structure Determination;Devonport, Jack;2021;Cambridge Crystallographic Data Centre


CCDC 2080823: Experimental Crystal Structure Determination;Devonport, Jack;2021;Cambridge Crystallographic Data Centre


CCDC 2080824: Experimental Crystal Structure Determination;Devonport, Jack;2021;Cambridge Crystallographic Data Centre


CCDC 2080825: Experimental Crystal Structure Determination;Devonport, Jack;2021;Cambridge Crystallographic Data Centre


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CCDC 2082797: Experimental Crystal Structure Determination;Fornier, Suzanne Daignan;2022;Cambridge Crystallographic Data Centre


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CCDC 2083057: Experimental Crystal Structure Determination;Zhang, Shan-Shan;2022;Cambridge Crystallographic Data Centre


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CCDC 2083313: Experimental Crystal Structure Determination;Kartal, Seda;2022;Cambridge Crystallographic Data Centre


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CCDC 2083926: Experimental Crystal Structure Determination;Poggini, Lorenzo;2021;Cambridge Crystallographic Data Centre


CCDC 2083927: Experimental Crystal Structure Determination;Poggini, Lorenzo;2021;Cambridge Crystallographic Data Centre