Experiment | |
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Method _exptl.method | X-RAY DIFFRACTION The method used in the experiment. |
Source type _diffrn_source.source | ROTATING ANODE The general class of the radiation source. |
Source details _diffrn_source.type | RIGAKU RUH2R The make, model or name of the source of radiation. |
Temperature [K] _diffrn.ambient_temp | 289 The mean temperature in kelvins at which the intensities were |
Detector technology _diffrn_detector.detector | IMAGE PLATE The general class of the radiation detector. |
Collection date _diffrn_detector.pdbx_collection_date | 1997-07-11 The date of data collection. |
Detector _diffrn_detector.type | RIGAKU RAXIS IIC The make, model or name of the detector device used. |
Software | |
Data reduction _software.classification | DENZO The classification of the program according to its |
Data scaling _software.classification | SCALEPACK The classification of the program according to its |
Phasing _software.classification | X-PLOR (3.851) The classification of the program according to its |
Model building _software.classification | X-PLOR (3.851) The classification of the program according to its |
Refinement _software.classification | X-PLOR (3.851) The classification of the program according to its |
General information | |
Spacegroup name _symmetry.space_group_name_H-M | P 43 21 2 Hermann-Mauguin space-group symbol. Note that the |
Unit cell parameters _cell.length_{a,b,c} _cell.angle_{alpha,beta,gamma} | 94.2 Unit-cell length a corresponding to the structure reported in 94.2 Unit-cell length b corresponding to the structure reported in 165.9 Unit-cell length c corresponding to the structure reported in 90.0 Unit-cell angle alpha of the reported structure in degrees. 90.0 Unit-cell angle beta of the reported structure in degrees. 90.0 Unit-cell angle gamma of the reported structure in degrees. |
Wavelength _diffrn_radiation_wavelength.wavelength | 1.54180 ÅThe radiation wavelength in angstroms. |
Data quality metrics | Overall |
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Low resolution limit [Å] _reflns.d_resolution_low | 100.000 The largest value in angstroms for the interplanar spacings |
High resolution limit [Å] _reflns.d_resolution_high | 2.000 The smallest value in angstroms for the interplanar spacings |
Rmerge _reflns.pdbx_Rmerge_I_obs | 0.065 The R value for merging intensities satisfying the observed |
Rmeas | - |
Rpim | - |
Total number of observations | - |
Total number unique _reflns.number_obs | 40863 The number of reflections in the REFLN list (not the DIFFRN_REFLN |
<I/σ(I)> _reflns.pdbx_netI_over_sigmaI | 12.00 The mean of the ratio of the intensities to their |
Completeness [%] _reflns.percent_possible_obs | 79.9 The percentage of geometrically possible reflections represented |
Multiplicity _reflns.pdbx_redundancy | 2.3 Overall redundancy for this data set. |
CC(1/2) | - |
Refinement | |
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PDB entry ID _entry.id | 1A95 |
Deposition date _pdbx_database_status.recvd_initial_deposition_date | 1998-04-16 |
Resolution _refine.ls_d_res_low _refine.ls_d_res_high | 50.0 - 2.000 Å |
Rwork/Rfree _refine.ls_R_factor_R_work _refine.ls_R_factor_R_free | 0.2070 / 0.2320 |
Structure solution method _refine.pdbx_method_to_determine_struct | MOLECULAR REPLACEMENT |
Starting model (for MR) _refine.pdbx_starting_model | 1NUL |