#------------------------------------------------------------------------------
#$Date: 2024-05-11 04:59:05 +0300 (Sat, 11 May 2024) $
#$Revision: 291821 $
#$URL: file:///home/coder/svn-repositories/cod/cif/1/57/16/1571601.cif $
#------------------------------------------------------------------------------
#
# This file is available in the Crystallography Open Database (COD),
# http://www.crystallography.net/. The original data for this entry
# were provided by IUCr Journals, http://journals.iucr.org/.
#
# The file may be used within the scientific community so long as
# proper attribution is given to the journal article from which the
# data were obtained.
#
data_1571601
loop_
_publ_author_name
'Zwolenik, A.'
'Tchoń, D'
'Makal, A.'
_publ_section_title
;
 Evolution of structure and spectroscopic properties of a new
 1,3-diacetylpyrene polymorph with temperature and pressure.
;
_journal_issue                   4
_journal_name_full               IUCrJ
_journal_paper_doi               10.1107/S2052252524003634
_journal_volume                  11
_journal_year                    2024
_chemical_formula_moiety         'C20 H14 O2'
_chemical_formula_sum            'C20 H14 O2'
_chemical_formula_weight         286.333
_space_group_crystal_system      monoclinic
_space_group_IT_number           14
_space_group_name_Hall           '-P 2ybc'
_space_group_name_H-M_alt        'P 1 21/c 1'
_symmetry_Int_Tables_number      14
_symmetry_space_group_name_Hall  '-P 2ybc'
_symmetry_space_group_name_H-M   'P 1 21/c 1'
_cell_angle_alpha                90
_cell_angle_beta                 101.697(3)
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   6.9685(2)
_cell_length_b                   10.7405(4)
_cell_length_c                   17.5252(6)
_cell_measurement_reflns_used    5171
_cell_measurement_temperature    298
_cell_measurement_theta_max      18.4030
_cell_measurement_theta_min      1.7740
_cell_volume                     1284.44(8)
_computing_cell_refinement       'CrysAlisPro 1.171.39.43d (Rigaku OD, 2018)'
_computing_data_collection       'CrysAlisPro 1.171.39.43d (Rigaku OD, 2018)'
_computing_data_reduction        'CrysAlisPro 1.171.39.43d (Rigaku OD, 2018)'
_computing_molecular_graphics    'Olex2 1.5-alpha (Dolomanov et al., 2009)'
_diffrn_ambient_temperature      298.15
_diffrn_crystal_treatment
'pressurized rapidly in silicone oil as a hydrostatic medium'
_diffrn_measured_fraction_theta_full 0.8194
_diffrn_measured_fraction_theta_max 0.7668
_diffrn_measurement_details
;
List of Runs (angles in degrees, time in seconds):

  # Type    Start    End  Width  tₑₓₚ   ω     θ     κ     φ   Frames
--------------------------------------------------------------------------
  1  ω    -43.00  41.00   1.00    1.00    --    0.00   0.00   0.00   84
  2  ω    -43.00  41.00   1.00    5.00    --    0.00   0.00   0.00   84
  3  ω    -43.00  41.00   1.00    1.00    --    0.00  30.00   0.00   84
  4  ω    -43.00  41.00   1.00    5.00    --    0.00  30.00   0.00   84
  5  ω    -43.00  41.00   1.00    1.00    --    0.00  90.00   0.00   84
  6  ω    -43.00  41.00   1.00    5.00    --    0.00  90.00   0.00   84
;
_diffrn_measurement_device_type
'esperanto-CrysAlisPro-abstract goniometer imported esperanto images'
_diffrn_radiation_type           synchrotron
_diffrn_radiation_wavelength     0.41618
_diffrn_reflns_av_R_equivalents  0.0828
_diffrn_reflns_av_unetI/netI     0.0342
_diffrn_reflns_Laue_measured_fraction_full 0.8194
_diffrn_reflns_Laue_measured_fraction_max 0.7668
_diffrn_reflns_limit_h_max       10
_diffrn_reflns_limit_h_min       -10
_diffrn_reflns_limit_k_max       14
_diffrn_reflns_limit_k_min       -14
_diffrn_reflns_limit_l_max       26
_diffrn_reflns_limit_l_min       -25
_diffrn_reflns_number            33624
_diffrn_reflns_point_group_measured_fraction_full 0.8194
_diffrn_reflns_point_group_measured_fraction_max 0.7668
_diffrn_reflns_theta_full        14.4602
_diffrn_reflns_theta_max         18.68
_diffrn_reflns_theta_min         1.75
_exptl_absorpt_coefficient_mu    0.041
_exptl_absorpt_correction_T_max  0.998
_exptl_absorpt_correction_T_min  0.998
_exptl_absorpt_correction_type   analytical
_exptl_absorpt_process_details
;
CrysAlisPro 1.171.39.43d (Rigaku Oxford Diffraction, 2018)
Analytical numeric absorption correction using a multifaceted crystal
   model based on expressions derived by R.C. Clark & J.S. Reid.
(Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897)
Empirical absorption correction using spherical harmonics,
 implemented in SCALE3 ABSPACK scaling algorithm.
;
_exptl_crystal_colour            'clear orange'
_exptl_crystal_colour_lustre     clear
_exptl_crystal_colour_primary    orange
_exptl_crystal_density_diffrn    1.481
_exptl_crystal_description       irregular
_exptl_crystal_F_000             600.009
_exptl_crystal_preparation
'Mounted in a Diamond-Anvil Cell using silicone oil as pressure medium.'
_exptl_crystal_pressure_history  'Pressurized to 0.85 GPa.'
_exptl_crystal_size_max          0.25
_exptl_crystal_size_mid          0.15
_exptl_crystal_size_min          0.1
_refine_diff_density_max         0.1950
_refine_diff_density_min         -0.2133
_refine_diff_density_rms         0.0519
_refine_ls_d_res_high            0.6497
_refine_ls_d_res_low             6.8238
_refine_ls_goodness_of_fit_ref   1.0541
_refine_ls_matrix_type           full
_refine_ls_number_constraints    0
_refine_ls_number_parameters     375
_refine_ls_number_reflns         3765
_refine_ls_number_restraints     0
_refine_ls_restrained_S_all      1.0541
_refine_ls_R_factor_all          0.0604
_refine_ls_R_factor_gt           0.0345
_refine_ls_shift/su_max          0.0006
_refine_ls_shift/su_mean         0.0000
_refine_ls_structure_factor_coef Fsqd
_refine_ls_weighting_details
'w=1/[σ²(Fo²)+(0.0308P)²+0.0330P] where P=(Fo²+2Fc²)/3'
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_gt          0.0695
_refine_ls_wR_factor_ref         0.0809
_reflns_Friedel_coverage         0.0
_reflns_limit_h_max              10
_reflns_limit_h_min              -10
_reflns_limit_k_max              14
_reflns_limit_k_min              0
_reflns_limit_l_max              26
_reflns_limit_l_min              0
_reflns_number_gt                2613
_reflns_number_total             3765
_reflns_threshold_expression     I>=2u(I)
_cod_data_source_file            yc5047.cif
_cod_data_source_block           2oAPb_0p85GPa_HAR_anh
_cod_database_code               1571601
_olex2_refine_details
;
Refinement using NoSpherA2, an implementation of
NOn-SPHERical Atom-form-factors in Olex2.
Please cite:
F. Kleemiss et al. Chem. Sci. DOI 10.1039/D0SC05526C - 2021
NoSpherA2 implementation of HAR makes use of
tailor-made aspherical atomic form factors calculated
on-the-fly from a Hirshfeld-partitioned electron density (ED) - not from
spherical-atom form factors.

The ED is calculated from a gaussian basis set single determinant SCF
wavefunction - either Hartree-Fock or DFT using selected funtionals
 - for a fragment of the crystal.
This fragment can be embedded in an electrostatic crystal field by 
employing cluster charges
or modelled using implicit solvation models, depending on the software used.
The following options were used:
   SOFTWARE:       ORCA 5.0
   PARTITIONING:   NoSpherA2
   INT ACCURACY:   Normal
   METHOD:         B3LYP
   BASIS SET:      6-311G(d,p)
   CHARGE:         0
   MULTIPLICITY:   1
   DATE:           2024-02-20_12-26-43
;
loop_
_space_group_symop_id
_space_group_symop_operation_xyz
1 x,y,z
2 -x,y+1/2,-z+1/2
3 -x,-y,-z
4 x,-y-1/2,z-1/2
loop_
_atom_site_label
_atom_site_type_symbol
_atom_site_fract_x
_atom_site_fract_y
_atom_site_fract_z
_atom_site_U_iso_or_equiv
_atom_site_adp_type
_atom_site_occupancy
O1 O 0.47665(19) 0.57598(13) 0.73751(7) 0.0487(4) Uani 1.000000
O2 O 0.2615(2) 0.08151(14) 0.47644(8) 0.0601(5) Uani 1.000000
C1 C 0.31998(10) 0.44362(8) 0.63490(5) 0.02973(17) Uani 1.000000
C2 C 0.29995(10) 0.52972(8) 0.57234(4) 0.02927(17) Uani 1.000000
C3 C 0.33273(12) 0.66074(9) 0.58334(6) 0.0371(2) Uani 1.000000
H3 H 0.3724(16) 0.6960(11) 0.6418(6) 0.069(3) Uani 1.000000
C4 C 0.31934(13) 0.74055(11) 0.52243(6) 0.0404(2) Uani 1.000000
H4 H 0.3515(17) 0.8401(13) 0.5322(7) 0.080(4) Uani 1.000000
C5 C 0.26744(11) 0.69718(9) 0.44414(5) 0.0366(2) Uani 1.000000
C6 C 0.26056(13) 0.77817(12) 0.38112(6) 0.0468(3) Uani 1.000000
H6 H 0.2951(18) 0.8764(14) 0.3928(7) 0.085(4) Uani 1.000000
C7 C 0.21089(13) 0.73366(12) 0.30529(6) 0.0509(3) Uani 1.000000
H7 H 0.2097(16) 0.7981(13) 0.2579(7) 0.080(4) Uani 1.000000
C8 C 0.16738(13) 0.60904(12) 0.29134(6) 0.0474(3) Uani 1.000000
H8 H 0.1274(17) 0.5720(12) 0.2323(7) 0.081(4) Uani 1.000000
C9 C 0.17491(11) 0.52521(10) 0.35298(5) 0.0378(2) Uani 1.000000
C10 C 0.13585(12) 0.39595(11) 0.34003(6) 0.0424(2) Uani 1.000000
H10 H 0.0945(17) 0.3638(12) 0.2808(6) 0.074(4) Uani 1.000000
C11 C 0.15038(12) 0.31437(11) 0.39985(5) 0.0394(2) Uani 1.000000
H11 H 0.1217(17) 0.2187(13) 0.3884(6) 0.069(3) Uani 1.000000
C12 C 0.20964(10) 0.35446(8) 0.47928(5) 0.03114(18) Uani 1.000000
C13 C 0.23365(10) 0.27104(8) 0.54285(5) 0.03209(18) Uani 1.000000
C14 C 0.28352(11) 0.31806(9) 0.61838(5) 0.03267(19) Uani 1.000000
H14 H 0.3029(14) 0.2539(10) 0.6664(6) 0.056(3) Uani 1.000000
C15 C 0.24301(9) 0.48398(8) 0.49460(5) 0.02905(17) Uani 1.000000
C16 C 0.22641(10) 0.56875(9) 0.43079(5) 0.03247(19) Uani 1.000000
C17 C 0.38966(12) 0.47976(10) 0.71804(5) 0.03432(19) Uani 1.000000
C18 C 0.35233(19) 0.39219(13) 0.78027(6) 0.0486(3) Uani 1.000000
H18a H 0.208(2) 0.3639(19) 0.7699(8) 0.129(7) Uani 1.000000
H18b H 0.391(3) 0.4356(14) 0.8346(7) 0.112(6) Uani 1.000000
H18c H 0.432(3) 0.3093(16) 0.7808(9) 0.127(7) Uani 1.000000
C19 C 0.22464(12) 0.13285(11) 0.53336(6) 0.0386(2) Uani 1.000000
C20 C 0.17274(18) 0.05592(13) 0.59787(7) 0.0476(3) Uani 1.000000
H20a H 0.051(2) 0.0922(15) 0.6172(11) 0.131(7) Uani 1.000000
H20b H 0.290(2) 0.0562(16) 0.6444(9) 0.120(6) Uani 1.000000
H20c H 0.142(3) -0.0362(17) 0.5796(10) 0.123(6) Uani 1.000000
loop_
_atom_type_symbol
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
_atom_type_scat_dispersion_source
C -0.00006 0.00048 'NoSpherA2: Chem.Sci. 2021, DOI:10.1039/D0SC05526C'
'Brennan, Cowan, Rev. Sci. Instrum., 1992, 63, 850'
H 0.00000 0.00000 'NoSpherA2: Chem.Sci. 2021, DOI:10.1039/D0SC05526C'
'Brennan, Cowan, Rev. Sci. Instrum., 1992, 63, 850'
O 0.00178 0.00185 'NoSpherA2: Chem.Sci. 2021, DOI:10.1039/D0SC05526C'
'Brennan, Cowan, Rev. Sci. Instrum., 1992, 63, 850'
loop_
_exptl_crystal_face_index_h
_exptl_crystal_face_index_k
_exptl_crystal_face_index_l
_exptl_crystal_face_perp_dist
1 25 9 0.0551
6 19 20 0.0500
-6 -19 -20 0.0500
12 12 13 0.0920
15 -2 11 0.0873
6 -24 -3 0.0883
0 -25 -9 0.0677
-8 -20 -13 0.0700
-13 13 -6 0.0830
loop_
_geom_angle_atom_site_label_1
_geom_angle_atom_site_label_2
_geom_angle_atom_site_label_3
_geom_angle
_geom_angle_site_symmetry_1
_geom_angle_site_symmetry_3
C14 C1 C2 119.04(7) . .
C17 C1 C2 123.15(8) . .
C17 C1 C14 117.72(8) . .
C3 C2 C1 123.23(7) . .
C15 C2 C1 118.56(8) . .
C15 C2 C3 118.21(8) . .
H3 C3 C2 118.5(6) . .
C4 C3 C2 122.06(9) . .
C4 C3 H3 119.4(7) . .
H4 C4 C3 120.8(7) . .
C5 C4 C3 120.97(10) . .
C5 C4 H4 118.2(7) . .
C6 C5 C4 121.23(10) . .
C16 C5 C4 118.70(8) . .
C16 C5 C6 120.07(9) . .
H6 C6 C5 118.8(6) . .
C7 C6 C5 120.23(12) . .
C7 C6 H6 121.0(6) . .
H7 C7 C6 118.5(8) . .
C8 C7 C6 120.36(10) . .
C8 C7 H7 121.1(8) . .
H8 C8 C7 121.7(7) . .
C9 C8 C7 120.92(10) . .
C9 C8 H8 117.4(7) . .
C10 C9 C8 121.89(9) . .
C16 C9 C8 119.55(10) . .
C16 C9 C10 118.55(8) . .
H10 C10 C9 118.1(7) . .
C11 C10 C9 121.70(9) . .
C11 C10 H10 120.2(7) . .
H11 C11 C10 120.0(6) . .
C12 C11 C10 121.22(10) . .
C12 C11 H11 118.7(6) . .
C13 C12 C11 122.63(9) . .
C15 C12 C11 118.61(8) . .
C15 C12 C13 118.75(7) . .
C14 C13 C12 119.09(8) . .
C19 C13 C12 123.15(8) . .
C19 C13 C14 117.56(8) . .
C13 C14 C1 123.27(8) . .
H14 C14 C1 118.0(6) . .
H14 C14 C13 118.6(6) . .
C12 C15 C2 121.24(7) . .
C16 C15 C2 119.40(8) . .
C16 C15 C12 119.32(7) . .
C9 C16 C5 118.87(8) . .
C15 C16 C5 120.60(8) . .
C15 C16 C9 120.50(9) . .
C1 C17 O1 122.85(10) . .
C18 C17 O1 118.69(10) . .
C18 C17 C1 118.45(10) . .
H18a C18 C17 111.3(8) . .
H18b C18 C17 109.4(8) . .
H18b C18 H18a 110.7(13) . .
H18c C18 C17 111.7(10) . .
H18c C18 H18a 104.2(15) . .
H18c C18 H18b 109.4(12) . .
C13 C19 O2 122.18(13) . .
C20 C19 O2 119.52(14) . .
C20 C19 C13 118.29(9) . .
H20a C20 C19 111.8(9) . .
H20b C20 C19 108.7(9) . .
H20b C20 H20a 107.7(15) . .
H20c C20 C19 110.8(9) . .
H20c C20 H20a 108.7(12) . .
H20c C20 H20b 109.0(13) . .
loop_
_geom_bond_atom_site_label_1
_geom_bond_atom_site_label_2
_geom_bond_distance
_geom_bond_site_symmetry_2
O1 C17 1.2117(14) .
O2 C19 1.2121(16) .
C1 C14 1.3918(12) .
C1 C2 1.4194(12) .
C1 C17 1.4909(11) .
C2 C15 1.4267(11) .
C2 C3 1.4324(13) .
C3 H3 1.074(10) .
C3 C4 1.3575(14) .
C4 H4 1.099(13) .
C4 C5 1.4245(13) .
C5 C6 1.3990(13) .
C5 C16 1.4185(13) .
C6 H6 1.092(15) .
C6 C7 1.3885(17) .
C7 H7 1.080(10) .
C7 C8 1.3831(17) .
C8 H8 1.090(12) .
C8 C9 1.3990(14) .
C9 C16 1.4172(12) .
C9 C10 1.4241(14) .
C10 H10 1.077(10) .
C10 C11 1.3543(15) .
C11 H11 1.058(13) .
C11 C12 1.4354(12) .
C12 C13 1.4130(12) .
C12 C15 1.4269(12) .
C13 C14 1.3934(12) .
C13 C19 1.4935(14) .
C14 H14 1.074(10) .
C15 C16 1.4284(12) .
C17 C18 1.5021(15) .
C18 H18a 1.029(13) .
C18 H18b 1.046(13) .
C18 H18c 1.048(16) .
C19 C20 1.5024(17) .
C20 H20b 1.029(13) .
C20 H20a 1.048(15) .
C20 H20c 1.049(17) .
loop_
_geom_torsion_atom_site_label_1
_geom_torsion_atom_site_label_2
_geom_torsion_atom_site_label_3
_geom_torsion_atom_site_label_4
_geom_torsion
_geom_torsion_site_symmetry_1
_geom_torsion_site_symmetry_2
_geom_torsion_site_symmetry_3
_geom_torsion_site_symmetry_4
O1 C17 C1 C2 -17.81(12) . . . .
O1 C17 C1 C14 158.62(11) . . . .
O2 C19 C13 C12 25.27(13) . . . .
O2 C19 C13 C14 -149.53(11) . . . .
C1 C2 C3 C4 177.62(8) . . . .
C1 C2 C15 C12 -1.02(8) . . . .
C1 C2 C15 C16 -178.58(7) . . . .
C1 C14 C13 C12 -2.97(9) . . . .
C1 C14 C13 C19 172.04(7) . . . .
C2 C3 C4 C5 1.37(9) . . . .
C2 C15 C12 C11 179.28(7) . . . .
C2 C15 C12 C13 0.11(8) . . . .
C2 C15 C16 C5 0.50(8) . . . .
C2 C15 C16 C9 178.40(7) . . . .
C3 C4 C5 C6 -177.58(8) . . . .
C3 C4 C5 C16 1.08(10) . . . .
C4 C5 C6 C7 179.56(8) . . . .
C4 C5 C16 C9 -179.94(7) . . . .
C4 C5 C16 C15 -2.00(8) . . . .
C5 C6 C7 C8 0.14(11) . . . .
C5 C16 C9 C8 0.57(8) . . . .
C5 C16 C9 C10 179.37(7) . . . .
C5 C16 C15 C12 -177.11(7) . . . .
C6 C7 C8 C9 -0.85(11) . . . .
C7 C8 C9 C10 -178.29(8) . . . .
C7 C8 C9 C16 0.48(10) . . . .
C8 C9 C10 C11 177.51(8) . . . .
C8 C9 C16 C15 -177.37(7) . . . .
C9 C10 C11 C12 -1.19(10) . . . .
C9 C16 C15 C12 0.80(8) . . . .
C10 C11 C12 C13 -177.46(8) . . . .
C10 C11 C12 C15 3.41(10) . . . .
C11 C12 C13 C14 -177.31(8) . . . .
C11 C12 C13 C19 7.97(9) . . . .
C11 C12 C15 C16 -3.16(8) . . . .
C12 C13 C19 C20 -156.25(8) . . . .
loop_
_atom_site_anharm_gc_c_label
_atom_site_anharm_gc_c_111
_atom_site_anharm_gc_c_112
_atom_site_anharm_gc_c_113
_atom_site_anharm_gc_c_122
_atom_site_anharm_gc_c_123
_atom_site_anharm_gc_c_133
_atom_site_anharm_gc_c_222
_atom_site_anharm_gc_c_223
_atom_site_anharm_gc_c_233
_atom_site_anharm_gc_c_333
O1 -0.000012(4) 0.0000001(12) 0.0000007(8) -0.0000000(7) 0.0000003(3)
0.0000001(3) -0.0000009(9) 0.0000000(2) 0.00000006(16) -0.00000002(19)
O2 -0.0000157(17) 0.0000013(6) 0.0000001(4) -0.0000001(3) 0.00000030(14)
0.00000011(14) -0.0000001(4) -0.00000020(11) 0.00000006(7) 0.00000001(9)
loop_
_atom_site_anharm_gc_d_label
_atom_site_anharm_gc_d_1111
_atom_site_anharm_gc_d_1112
_atom_site_anharm_gc_d_1113
_atom_site_anharm_gc_d_1122
_atom_site_anharm_gc_d_1123
_atom_site_anharm_gc_d_1133
_atom_site_anharm_gc_d_1222
_atom_site_anharm_gc_d_1223
_atom_site_anharm_gc_d_1233
_atom_site_anharm_gc_d_1333
_atom_site_anharm_gc_d_2222
_atom_site_anharm_gc_d_2223
_atom_site_anharm_gc_d_2233
_atom_site_anharm_gc_d_2333
_atom_site_anharm_gc_d_3333
O1 0.0000006(5) -0.00000009(16) 0.00000004(10) -0.00000000(8) -0.00000001(3)
0.00000001(3) 0.00000001(6) 0.000000009(19) -0.000000007(11) -0.000000007(14)
-0.00000011(8) -0.000000002(18) 0.000000007(10) -0.000000003(7) -0.000000008(10)
O2 0.0000006(3) -0.00000012(7) 0.00000012(5) -0.00000000(4) -0.000000019(15)
0.000000033(15) -0.00000001(3) 0.000000001(9) -0.000000003(5) 0.000000008(7)
-0.00000014(4) 0.000000003(8) 0.000000006(5) -0.000000001(3) -0.000000012(5)
