Data quality metrics extracted from 9nzn.cif.gz by aB_cif2table1 from BUSTER (Global Phasing Ltd.). See also the PDBx/mmCIF dictionary and a MXLIMS-compatible JSON representation.


Experimental information for 9NZN at RCSB, PDBe, PDBj

Experiment
Method
_exptl.method
X-RAY DIFFRACTION
Experimental protocol
_diffrn_radiation.pdbx_diffrn_protocol
SINGLE WAVELENGTH
Source type
_diffrn_source.source
SYNCHROTRON
Source details
_diffrn_source.type
NSLS-II BEAMLINE 17-ID-1
Synchrotron site
_diffrn_source.pdbx_synchrotron_site
NSLS-II
Beamline
_diffrn_source.pdbx_synchrotron_beamline
17-ID-1
Temperature [K]
_diffrn.ambient_temp
100
Detector technology
_diffrn_detector.detector
PIXEL
Collection date
_diffrn_detector.pdbx_collection_date
2023-01-29
Detector
_diffrn_detector.type
DECTRIS EIGER X 9M
Wavelength(s) [Å]
_diffrn_source.pdbx_wavelength_list
0.92000
Software
Data processing
_software.classification
autoPROC ()
Data reduction
_software.classification
XDS (Jan 10, 2022; 2022-02-20)
Data scaling #1
_software.classification
Aimless (0.7.8; 20210728)
Data scaling #2
_software.classification
STARANISO (2.3.87; 2.3.87 (18-05-2022))
Phasing
_software.classification
AMoRE
Refinement
_software.classification
BUSTER (2.11.8; 2022-11-21)
General information
Spacegroup name
_symmetry.space_group_name_H-M
P 21 21 21
Unit cell parameters
_cell.length_{a,b,c} _cell.angle_{alpha,beta,gamma}
40.095 50.928 90.182 90.0 90.0 90.0
Wavelength
_diffrn_radiation_wavelength.wavelength
0.92000 Å

Diffraction limits
_reflns.pdbx_aniso_diffraction_limit_{1,2,3}
Principal axes of ellipsoid fitted to diffraction cut-off surface
_reflns.pdbx_aniso_diffraction_limit_axis_{1,2,3}_ortho[1..3]
1.504 Å 1.0000 0.0000 0.0000
1.530 Å 0.0000 0.0000 0.0000
1.584 Å 0.0000 0.0000 0.0000

Criteria used in determination of diffraction limits:
local <I/sigmaI>1.20

Data quality metricsOverallInnerShellOuterShell
Low resolution limit [Å]
_reflns.d_resolution_low _reflns_shell.d_res_low
45.091 45.091 1.591
High resolution limit [Å]
_reflns.d_resolution_high _reflns_shell.d_res_high
1.504 4.430 1.504
Rmerge
_reflns.pdbx_Rmerge_I_obs _reflns_shell.Rmerge_I_obs
0.082 0.052 0.989
Rmeas
_reflns.pdbx_Rrim_I_all _reflns_shell.pdbx_Rrim_I_all
0.086 0.055 1.100
Rpim
_reflns.pdbx_Rpim_I_all _reflns_shell.pdbx_Rpim_I_all
0.024 0.015 0.466
Total number of observations
_reflns.pdbx_number_measured_all _reflns_shell.number_measured_all
294191 15997 6895
Total number unique
_reflns.number_obs _reflns_shell.number_unique_all
25968 1298 1299
<I/σ(I)>
_reflns.pdbx_netI_over_sigmaI _reflns_shell.meanI_over_sigI_obs
14.92 39.89 1.34
Completeness (spherical) [%]
_reflns.pdbx_percent_possible_spherical _reflns_shell.pdbx_percent_possible_spherical
86.4 99.8 28.5
Completeness (ellipsoidal) [%]
_reflns.pdbx_percent_possible_ellipsoidal _reflns_shell.pdbx_percent_possible_ellipsoidal
91.8 99.8 43.9
Multiplicity
_reflns.pdbx_redundancy _reflns_shell.pdbx_redundancy
11.3 12.3 5.3
CC(1/2)
_reflns.pdbx_CC_half _reflns_shell.pdbx_CC_half
0.999 0.998 0.521
Anomalous completeness (spherical)
_reflns.pdbx_percent_possible_spherical_anomalous _reflns_shell.pdbx_percent_possible_spherical_anomalous
86.3 100.0 30.2
Anomalous completeness (ellipsoidal)
_reflns.pdbx_percent_possible_ellipsoidal_anomalous _reflns_shell.pdbx_percent_possible_ellipsoidal_anomalous
91.9 100.0 45.9
Anomalous multiplicity
_reflns.pdbx_redundancy_anomalous _reflns_shell.pdbx_redundancy_anomalous
6.0 7.3 2.7
CC(ano)
_reflns.pdbx_CC_half_anomalous _reflns_shell.pdbx_CC_half_anomalous
-0.100 -0.075 -0.076
|DANO|/σ(DANO)
_reflns.pdbx_absDiff_over_sigma_anomalous _reflns_shell.pdbx_absDiff_over_sigma_anomalous
0.733 0.753 0.647

Refinement
PDB entry ID
_entry.id
9NZN
Deposition date
_pdbx_database_status.recvd_initial_deposition_date
2025-04-01
Resolution
_refine.ls_d_res_low _refine.ls_d_res_high
17.5 - 1.504 Å
Rwork/Rfree
_refine.ls_R_factor_R_work _refine.ls_R_factor_R_free
0.2055 / 0.2242
Structure solution method
_refine.pdbx_method_to_determine_struct
MOLECULAR REPLACEMENT
Starting model (for MR)
_refine.pdbx_starting_model
WARNING: no starting model (for MR) given