Experiment | |
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Method _exptl.method | X-RAY DIFFRACTION The method used in the experiment. |
Experimental protocol _diffrn_radiation.pdbx_diffrn_protocol | SINGLE WAVELENGTH SINGLE WAVELENGTH, LAUE, or MAD. |
Source type _diffrn_source.source | SYNCHROTRON The general class of the radiation source. |
Source details _diffrn_source.type | APS BEAMLINE 32-ID The make, model or name of the source of radiation. |
Synchrotron site _diffrn_source.pdbx_synchrotron_site | APS Synchrotron site. |
Beamline _diffrn_source.pdbx_synchrotron_beamline | 32-ID Synchrotron beamline. |
Detector technology _diffrn_detector.detector | CCD The general class of the radiation detector. |
Collection date _diffrn_detector.pdbx_collection_date | 2003-12-01 The date of data collection. |
Detector _diffrn_detector.type | MARRESEARCH The make, model or name of the detector device used. |
Wavelength(s) [Å] _diffrn_source.pdbx_wavelength_list | 0.97921 Comma separated list of wavelengths or wavelength range. |
Software | |
Data reduction _software.classification | DENZO (Zbyszek Otwinowski; zbyszek@mix.swmed.edu) The classification of the program according to its |
Data scaling _software.classification | SCALEPACK (Zbyszek Otwinowski; zbyszek@mix.swmed.edu) The classification of the program according to its |
Phasing #1 _software.classification | SOLVE (2.02; 29-Jan-2002; Tom Terwilliger; terwilliger@LANL.gov) The classification of the program according to its |
Phasing #2 _software.classification | RESOLVE (2.02; 08-Feb-2001; Terwilliger, T. C; terwilliger@LANL.gov) The classification of the program according to its |
Refinement _software.classification | REFMAC (refmac_5.1.24; 24/04/2001; Murshudov, G.N.; ccp4@dl.ac.uk) The classification of the program according to its |
General information | |
Spacegroup name _symmetry.space_group_name_H-M | P 1 2 1 Hermann-Mauguin space-group symbol. Note that the |
Unit cell parameters _cell.length_{a,b,c} _cell.angle_{alpha,beta,gamma} | 45.681 Unit-cell length a corresponding to the structure reported in 34.261 Unit-cell length b corresponding to the structure reported in 78.597 Unit-cell length c corresponding to the structure reported in 90.000 Unit-cell angle alpha of the reported structure in degrees. 90.008 Unit-cell angle beta of the reported structure in degrees. 90.000 Unit-cell angle gamma of the reported structure in degrees. |
Wavelength _diffrn_radiation_wavelength.wavelength | 0.97921 ÅThe radiation wavelength in angstroms. |
Data quality metrics | Overall | InnerShell | OuterShell |
---|---|---|---|
Low resolution limit [Å] _reflns.d_resolution_low _reflns_shell.d_res_low | 30.000 The largest value in angstroms for the interplanar spacings | 30.000 The highest value in angstroms for the interplanar spacings | 2.140 The highest value in angstroms for the interplanar spacings |
High resolution limit [Å] _reflns.d_resolution_high _reflns_shell.d_res_high | 2.100 The smallest value in angstroms for the interplanar spacings | 5.690 The smallest value in angstroms for the interplanar spacings | 2.100 The smallest value in angstroms for the interplanar spacings |
Rmerge _reflns.pdbx_Rmerge_I_obs _reflns_shell.Rmerge_I_obs | 0.065 The R value for merging intensities satisfying the observed | 0.067 The value of Rmerge(I) for reflections classified as 'observed' | 0.100 The value of Rmerge(I) for reflections classified as 'observed' |
Rmeas | - | - | - |
Rpim | - | - | - |
Total number of observations | - | - | - |
Total number unique _reflns.number_obs | 14582 The number of reflections in the REFLN list (not the DIFFRN_REFLN | - | - |
<I/σ(I)> | - | - | - |
Completeness [%] _reflns.percent_possible_obs | 99.8 The percentage of geometrically possible reflections represented | - | - |
Multiplicity | - | - | - |
CC(1/2) | - | - | - |
Refinement | |
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PDB entry ID _entry.id | 1VJH |
Deposition date _pdbx_database_status.recvd_initial_deposition_date | 2004-02-20 |
Resolution _refine.ls_d_res_low _refine.ls_d_res_high | 21.9 - 2.100 Å |
Rwork/Rfree _refine.ls_R_factor_R_work _refine.ls_R_factor_R_free | 0.1857 / 0.2392 |