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core CIF discussion #6

  • To: coredmg@iucr.org
  • Subject: core CIF discussion #6
  • From: David Brown <idbrown@mcmaster.ca>
  • Date: Mon, 26 Apr 2004 12:00:11 -0400
Core CIF Discussion #6

Dear Colleagues,

     I enclose below Discussion Paper #6 in the current round of changes
proposed for the core CIF dictionary.  This round contains five items 
from the
Discussion paper #5 with recommendations for the approval of some items and
dropping of others.  There is also a new item proposed by David Watkin for
recording information about refinements using distributed scattering density
such as a rotating ring of charge.

     This email prints out on around 17 pages.  Can you please check through
the items presented and send your comments to the core CIF discussion 
group at
coredmg@iucr.org?  I will start working on the next round after June 30 
which
is therefore the deadline for receiving comments.  If you need more time let
me know.  The deadline is flexible.

Best wishes

David Brown

-------------------------
General comment by Curt Haltiwanger
-----------------------------------
My perspective on cifs in general is  -
The cif should be a useful tool that allows a crystallographer to store
details of the experiment and to evaluate the quality of a reported result.
The cif must also allow crystallographers and other scientists access to the
data in a useful interpretable way for statistical studies.

My responses are driven by this perspective and my experience in single
crystal x-ray diffraction. I'd be interested in hearing the official mission
statement.  I wonder how close I am.  ???

Response by IDB.
----------------
I am not sure that there is an official mission statement for CIF but Curt's
summary is as good as any.  The nearest official mission statements I 
can find
are found in the original paper by Hall, Allen and Brown Acta Cryst. (1991)
A47, 655-685:

'In addition to archiving data, the use of a universal file would facilitate
data exchange between software within a laboratory; between different
laboratories; between authors and journals, providing electronic input 
to the
publication process; and between researchers or journals and computerized
databases.'

and in Syd Hall's account of the STAR file structure (J. Chem. Inf. 
Comp. Sci.
(1991) 31, 326-333) the properties of a STAR file are given as:

     'The data structure is completely self-defined
     The data items are completely self-defined
     The syntax rules are few and simple
     The data may be in any type and in any order
     The file is easy to read visually or by machine'

Perhaps between the three statements one can distill the flavour of CIF.

####################
#
# Items included below                     Recommendation
# -----------------------------------------------------------------
#
# Item 6 Atom_site_refinement_flag_        Editorial changes only
#
# Item 7 diffrn_refln_status               Drop
#
# Item 8 _geom_bond_count                  Approve
#
# Item 9 _refine_scattering_density        Drop
#
# Item 10 _atomic_sites_solution_hydrogen  Approve
#
# NEW ITEM
#
# Item 11  Distributed scattering density  Discussion
#
##########################################
#
# Item 6.
#
##########################################
#
# _atom_site_refinement_flag_adp
#
# Carried over from discussion #4
#
# There has been extensive discussion of this item which is designed to
# indicate the constraints or restraints applied to the ADP.  On one 
hand, it
# has been suggested that we should define a sufficient number of flags that
# someone could repeat the refinement.  On the other hand, there are so many
# different ways of applying restraints that enumerating all the 
possibilities
# becomes impossible.  All we can reasonably do is place a flag to warn the
# reader that at least some parameters were not freely refined, leaving
# further details to be given in the existing items 
_atom_site_constraint and
# _atom_site_restraint for individual atoms, or _refine_special_details 
for a
# more general description.
#
# Curt Haltiwanger (04-02-27) has written at length on this matter, and I
# extract part of his comment (his full comment is available as part of our
# discussion on the IUCr web site).
#
# Curt writes:
# ------------
# 'However I am having trouble figuring out whether the Uiso on a hydrogen
# atom that is set to 1.2 time the Ueq of the atom it is attached to 
would be
# constraint or a restraint or something else.   This is common situation in
# many or most structures with C-H's refined with SHELXL.  As I see it this
# treatment of hydrogen atoms does not fit either of the definitions for
# constraints and restraints.  I think it is important that we provide data
# items that allow users to report what they actually do.....
#
# I think it would be quite useful to have an official cif entry similar to
# _refinement_special_details, that would contain a copy of the refinement
# input file.  Would _refinement_input_file be a possibility?  I realize 
that
# this file would be of no use to anyone who did not have access to that
# particular program or to a users manual for the program.  I think it 
is much
# more significant that the scientist who did have access to the program or
# manuals would have access to the information that it is almost impossible
# for the cif to capture.  If someone did not have immediate access, they
# would still have the option of getting a version of the program.  At least
# the details would be present and the devil is in the details.
#
# 'So I don't think that we have exactly the right definition yet.  And I
# think that we need a way of including input files in the cif.'
#
# IDB Response:
# -------------
# The person preparing a CIF has the option to put anything they like in the
# various special_details and similar text fields, including the input 
file to
# the program they used, though a verbal description of the procedure 
would be
# more informative since it would be intelligible to people who did not have
# access to the program.  I list below some of the items that are already in
# the approved core dictionary, and these would seem to provide sufficient
# opportunities for recording the restraints and constraints applied during
# refinement.  In the interests of keeping things simple, I recommend 
that we
# make no change to these items (except for the editorial changes noted).
#
# The following seven items are taken from the latest approved coreCIF
# dictionary (version 2.3).  They provide plenty of space to describe a
# variety of different kinds of restraints.  Some possible editorial changes
# are suggested.
#
data_atom_site_refinement_flags_adp
    _name                      '_atom_site_refinement_flags_adp'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    _related_item              '_atom_site_refinement_flags'
    _related_function            alternate
    loop_ _enumeration
          _enumeration_detail
        .  'no constraints on atomic displacement parameters'
        T  'special-position constraints on atomic displacement parameters'
        U  'Uiso or Uij restraint (rigid bond)'
#
# A better _enumeration_detail for the above line might be:
# ; A restraint or constraint not related to symmetry applied to the atomic
# displacement parameters.
# ;
#
        TU 'Both constraints applied'
    _definition
;              A code which indicates the refinement restraints or 
constraints
               applied to the atomic displacement parameters of this site.
;
#
# The definition might better read 'A code that indicates that refinement
# restraints or constraints were applied...'
#

data_atom_site_refinement_flags_occupancy
    _name                      '_atom_site_refinement_flags_occupancy'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    _related_item              '_atom_site_refinement_flags'
    _related_function            alternate

   loop_ _enumeration
     _enumeration_detail   . 'no constraints on site occupancy parameters'
                           P 'site occupancy constraint'
    _definition
;              A code which indicates that refinement restraints or
               constraints were applied to the occupancy of this site.
;

data_atom_site_refinement_flags_posn
    _name                      '_atom_site_refinement_flags_posn'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    _related_item              '_atom_site_refinement_flags'
    _related_function            alternate
    loop_ _enumeration
          _enumeration_detail
                     . 'no constraints on  positional coordinates'
                     D 'distance or angle restraint on positional 
coordinates'
                     G 'rigid group refinement of positional coordinates'
                     R 'riding-atom site attached to non-riding atom'
                     S 'special position constraint on positional 
coordinates'
                     DG   'combination of the above constraints'
                     DR   'combination of the above constraints'
                     DS   'combination of the above constraints'
                     GR   'combination of the above constraints'
                     GS   'combination of the above constraints'
                     RS    'combination of the above constraints'
                     DGR  'combination of the above constraints'
                     DGS  'combination of the above constraints'
                     DRS  'combination of the above constraints'
                     GRS  'combination of the above constraints'
                     DGRS 'combination of the above constraints'
    _definition
;              A code which indicates the refinement restraints or 
constraints
               applied to the positional coordinates of this site.
;

data_atom_site_calc_attached_atom
    _name                      '_atom_site_calc_attached_atom'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
#
# This item should be shown as being a child of _atom_site_label
#
    _enumeration_default        '.'
    _definition
;              The _atom_site_label of the atom site to which the 'geometry-
               calculated' atom site is attached.
;

data_atom_site_calc_flag
    _name                      '_atom_site_calc_flag'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    loop_ _enumeration

      _enumeration_detail   d     'determined from diffraction measurements'
                            calc  'calculated from molecular geometry'
                            c     'abbreviation for "calc"'
                            dum   'dummy site with meaningless coordinates'
    _enumeration_default    d
    _definition
;              A standard code to signal if the site coordinates have been
               determined from the intensities or calculated from the 
geometry
               of surrounding sites, or have been assigned dummy 
coordinates.
               The abbreviation 'c' may be used in place of 'calc'.
;

data_atom_site_constraints
    _name                      '_atom_site_constraints'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    _enumeration_default        '.'
    _example                    'pop=1.0-pop(Zn3)'
    _definition
;              A description of the constraints applied to parameters at 
this
               site during refinement. See also _atom_site_refinement_flags
               and _refine_ls_number_constraints.
;

data_atom_site_restraints
    _name                      '_atom_site_restraints'
    _category                    atom_site
    _type                        char
    _list                        yes
    _list_reference            '_atom_site_label'
    _example                    'restrained to planar ring'
    _definition
;              A description of restraints applied to specific parameters at
               this site during refinement. See also
               _atom_site_refinement_flags and _refine_ls_number_restraints.
;
#
# The above two items should reference each other in the definition
#
# STATUS: Recommend only editorial changes
#

#######################################
#
# Item 7
#
#######################################
#
# _diffrn_refln_status
#
# COMMENT: The purpose of this proposed item is to allow reflections 
that are
# believed to be systematically absent during measurement to be flagged, but
# the question was raised, 'Where do we identify the assumed space group and
# in any cases does this flag make any sense?'
#
# Note that there is already an item _refln_refinement_status with 
values of:
# incl(uded in refinement), excl(uded from refinement) and extn 
(extinguished,
# i.e. systematically absent.  This flag is based on the space group used in
# the refinement and reported in the CIF.
#
# There is a persuasive lack of enthusiasm for this item and I propose 
that we
# drop it.  For this reason I have commented out the definition below.  I
# have, however, included an extract from Curt's comments at the end of this
# section where he raises another question.
#
#data_diffrn_refln_status
#_name                  '_diffrn_refln_status'
#_category              diffrn_refln
#_type                  char
#_list                  yes
#_list_reference        '_diffrn_refln_index_'
#loop_
#_enumeration
#_enumeration_detail
#        incl          'Reflection expected to have non-zero intensity'
#        sysabs        'Reflection considered to be systematically absent'
#_example               ?
#_definition
#;             A flag indicating whether a reflection was assumed to be
#              systematically absent during the measurement of the 
diffraction
#              intensities.
#;
#
# COMMENT by Curt Haltiwanger 04-02-27
# ------------------------------------
# As I write this, the most probable use that occurs to me would be if 
someone
# was using the cif to store all of the reflection data as input to the next
# step in the data processing and structure solution process.  If that 
is the
# case then there are other items that would be interesting, x,y position on
# the detector, frame and angle info, etc. I don't think that is a direction
# that we want to go.
#
# RESPONSE by IDB 04-03-05
#-------------------------
# There is already an image dictionary for reporting the contents of an two-
# dimensional diffraction image.  This is written in DDL2 but could be
# converted to DDL1 if there were a demand.
#
# STATUS: Recommend that this item be dropped (unless there is an outcry)
#-----------------------------------------------------
#
##########################################
#
# Item 8
#
##########################################
#
# _geom_bond_multiplicity
#
# COMMENT: In high symmetry structures when many bonds are related by 
symmetry
# it is not necessary to list all the bonds in the environment of the first
# named atom. Some users may wish to give only the symmetry independent
# distances and a multiplier to indicate how many such bonds are found 
in the
# atomic environment.  This is the way in which bond lengths are 
published in
# Acta Cryst.
#
# COMMENT by Howard Flack 04-01-14
# --------------------------------
#     OK with me
#
# COMMENT by Curt Haltwanger 04-02-27
# -----------------------------------
# I associate bond multiplicity with single and double bonds.  Perhaps 
that is
# more correctly referred to as bond order, but multiplicity seems to 
have the
# possibility of being confusing. IUPAC defines Multiplicity as "The 
existence
# of several degenerate wavefunctions distinguished only by the relative
# orientation of the angular spin momentum. Defined by the total angular 
spin
# momentum S, it is given by 2S+1."  Whatever that means.
# How about _geom_bond_symm_count instead of _geom_bond_multiplicity
#
# RESPONSE by IDB 04-03-05
# ------------------------
# In the draft dictionary text below I have changed the name to
# _geom_bond_count.  It is not necessary to include '_symm' since in almost
# all cases if two bonds have exactly the same length they will be 
related by
# symmetry.  We will need a corresponding item for angles.
#
data_geom_bond_count
_name               '_geom_bond_count'
_category           geom_bond
_type               numb
_list               yes
_list_reference     '_geom_bond_atom_site_label_'
loop_
    _example
    _example_detail
;      loop_
       _geom_bond_atom_site_label_1
       _geom_bond_atom_site_label_2
       _geom_bond_distance
       _geom_bond_count
           Ni1 O1 1.789(3) 4
           Ni1 O2 2.134(3) 2
;
       'Gives the lengths of the six bonds around Ni1'

_enumeration_range 0:
_definition
;          The number of times the given bond appears in the environment
           of the atoms labelled _geom_bond_atom_site_label_1. This should
           not be used if symmetry equivalent bonds are included explicitly
           in the list.
;
#
# STATUS: Ready for approval
#
##########################################
#
# Item 9
#
##########################################
#
# Category refine_scattering_density
#
# COMMENT
# -------
# The current dictionary has items that give the maximum and minimum 
values of
# the difference scattering density. Users are encouraged to identify the
# positions of the maximum and minimum in a _*_details item.
#
# There are occasions when one might wish to give a list of peaks in an 
x-ray,
# electron or neutron scattering density map together with their positions.
# This category is designed to hold this information.
#
# COMMENT from Curt Haltiwanger 04-02-27
# --------------------------------------
# It is important to distinguish between electron density and electron 
density
# map peaks.  Most programs and their users look only at peaks.  Large 
regions
# of diffuse electron density (solvent columns and solvent molecules in 
large
# holes come to mind) can be very hard to identify and describe.  If we are
# going to come up with definitions to describe electron density, we need to
# consider ways to deal with diffuse density.
# I cannot tell from the discussion here so far what information we are
# trying to capture.  I thought initially that this would be a way to give
# more details regarding residual difference electron density peaks, but 
from
# the definitions difference density peaks are not included at all.  Does
# anyone calculate refined scattering density?  Is this essentially what 
x-ray
# folks would call an electron density map or an Fo map? 
# I believe current accepted practice is to calculate a final difference 
map.
# It makes sense to me to report the position and height of the largest 
peaks
# and holes.  I look forward to hearing more discussion of this. 
#
# COMMENT from Howard Flack 04-01-14
# ----------------------------------
#     It seems to me that you need some more input from the people who
# requested this item to know whether they want full, difference, partial
# difference etc. I don't like the idea of a default radiation probe.
#
# RESPONSE by IDB.
# ----------------
# I cannot recall who asked for this item but there seems to be a sufficient
# number of complications that we should drop this item until we get a clear
# request stating exactly what is needed and why.  I have left in the 
comments
# that have been made since the previous discussion paper to illustrate some
# of the problems.
#
#data_refine_scattering_density_[]
#_name                    refine_scattering_density
#_category                null
#_type                    category_overview
#_example
#;            loop_
#             _refine_scattering_density_id
#             _refine_scattering_density_position_x
#             _refine_scattering_density_position_y
#             _refine_scattering_density_position_z
#             _refine_scattering_density_peak
#             _refine_scattering_density_details
#                1 0.0743 0.3568 0.4215 45.6 'probably Mo'
#                2 0.7358 0.2987 0.8932 43.2 'probably Mo'
#                3 0.8657 0.4518 -0.0654 25.8 ?
#;
#_definition
#; This is a category in which the peak positions and heights in
#the experimental scattering density map can be reported. The
#nature of the scattering density is determined by the radiation
#given in _diffrn_radiation_probe.
#;
#
# QUERY
# -----
# _diffrn_radiation_probe is not always given. Should it have a default 
value
# of 'x-ray'?
#
# REPLY by Curt Haltiwanger 04-02-27
#--------------------------
# >>>>>>>>>> Is a wavelength always [given] for x-ray experiments? 
# >>>>>>>>>> Could the default be determined on the basis of the 
wavelength or
# lack thereof?
#
#data_refine_scattering_density_details
#_name                   '_refine_scattering_density_details'
#_category               refine_scattering_density
#_type                   char
#_list                   yes
#_list_reference         '_refine_scattering_density_details
#loop_ _example          'Probably Mo'
#                        'Uncertain peak'
#                        'Broad diffuse peak'
#_definition
#;                A description of the scattering density peak
#;
#
#data_refine_scattering_density_id
#_name                   '_refine_scattering_density_id'
#_category               refine_scattering_density
#_type                   char
#_list                   yes
#_list_mandatory         yes
#_example                ?
#_definition
#;          A code identifying this particular scattering density peak.
#;
#
#
#data_refine_scattering_density_peak
#_name                   '_refine_scattering_density_peak'
#_category               refine_scattering_density
#_type                   numb
#_list                   yes
#_list_reference         '_refine_scattering_density_id'
#loop_
#_units
#_units_detail
#     e.A-3      'electrons per cubic angstrom for x-ray diffraction'
#     ?          'for neutron diffraction'
#     ?          'for electron diffraction'
#     e.A-3      'electrons per cubic angstrom for gamma ray diffraction'
#_example        ?
#_definition
#;               The measured scattering density at the given position. The
#                units are determined by the value of 
_diffrn_radiation_probe.
#;
#
#data_refine_scattering_density_position_
#loop_
#_name                 _refine_scattering_density_position_x
#                      _refine_scattering_density_position_y
#                      _refine_scattering_density_position_z
#_category             refine_scattering_density
#_type                 num
#_type_conditions      esd
#_list                 yes
#_list_reference       _refine_scattering_density_id
#_example ?
#_definition
#;                 The positional coordinates in fractions of the unit 
cell at
#                  which the electron density peak occurs.
#;
#
# QUERY: The definitions above imply the full scattering density. Should we
# make provision of the difference density to be given instead or as 
well as?
#
# REPLY by Curt 04-02-27
#>>>>>>>>>> I would say yes definitely.  I think this is the most likely use
# of such data.
#
# QUERY: Should there be provision for partial difference maps, i.e., maps
# with only some atoms removed? How should this be done?
#
# REPLY by Curt 04-02-27
#>>>>>>>> I don't think this is needed as a separate definition.
# If the cif has a list of atoms and a difference density peaks are reported
# then the difference peaks are what is left.  If electron density peaks are
# reported then they should be for all reported atoms plus any big peaks 
that
# are in the list.  But doesn't this open up another of these things that
# could get out of hand.  What about 2Fo - Fc maps?  Do we expect the 
user to
# report the cut off criteria.  I think it goes back to who is going to use
# this for what.  For the majority of small molecule scientists, this will
# never get used or will be used only for difference peaks.
#
# STATUS: Recommend this be dropped (unless there is an outcry)
#
#################################
#
# Item 10.
#
#################################
#
# _atomic_sites_solution_hydrogens
#
# COMMENT: The definition of this item in the current dictionary is bundled
# with primary and secondary solution methods
# and for this reason there is no flag to indicate that the hydrogen atoms
# were not located. We need a new flag for this case.
#
# Add to the enumeration loop the following
#
#       notdet 'coordinates were not determined'
#
# COMMENT by Howard Flack 04-01-14
# --------------------------------
#      OK with me.
#
# STATUS: Ready for approval
#
#####################################
#
# Item 11 Distributed scattering density
#
#####################################
#
# The following items are based on a request from David Watkin and are newly
# introduced into our discussion.  They are intended to describe electron
# density (or other scattering density) that is not in the form of a 
spherical
# atom, e.g., a ring of density arising from a rotating group such as a
# trifluooromethyl group or a cyclopentadiene molecule. 
#
# Various possible shapes are defined - ring, spherical shell,
# cylindrical shell, etc.  The atoms that form the ring or shell are listed
# with dummy coordinates in the atom_site loop, but flagged with an 
identifier
# that links them to a new category giving details of the shape of the
# distribution.  This requires an _*_distributed_density_id item in the
# atom_site category, and the definition of a new distributed_density
# category.
#
data__atom_site_distributed_density_id
    _name               '_atom_site_distributed_density_id'
    _category           atom_site
    _type               char
    _list               yes
    _list_reference     '_atom_site_label'
    _list_mandatory     no
    _link_parent        '_distributed_density_id'
    _example            ?
    _definition
;              An identifier that links the atom defined by _atom_site_label
               with a distributed density defined in the distributed_density
               category.  Note that all the atoms that give rise to the
               distributed density should be included in the atom_site list,
               even when they, or the centroid of the distribution, lie on a
               special position.  The value of
               _atom_site_symmetry_multiplicity should be chosen so that the
               sum of all the atoms multiplied by their symmetry 
multiplicity
               equals the chemical formula multiplied by Z.
;
#
#
##########################
#
#   New Category  DISTRIBUTED DENSITY
#
##########################
#
data_distributed_density_[]
    _name               '_distributed_density_[]
    _category           category_overview
    _type               null
    _definition
;              Items in the distributed density category describe the
               geometric arrangement of an atom or atoms when they are
               distributed uniformly over a line or surface such as a ring,
               cylinder or sphere.
;
loop_     _example_detail
          _example
;
This is a fictitious (and chemically implausible) example designed to
illustrate how a complex system of distributed density can be recorded.  In
this example pentamethyl cyclopentadiene (Cp*) and borazole occupy the same
location in the crystal in the ratio 5:1.  The atoms of the borazole 
ring are
fixed but one quarter of the Cp* molecules are freely rotating, while the
other three quarters occupy fixed positions.  The rotating Cp* molecules 
give
rise to two concentric rings of density, one from the atoms in the ring and
the other from the methyl groups.  On top of these rings lie the atoms 
of the
fixed Cp* molecules.  The atoms of the borazole molecule also lie over the
inner Cp* ring.  Full details of the chemical composition are given in the
atom_site loop together with the positions of the fixed atoms.  Note 
that the
coordinates of the atoms that give rise to the distributed ring of 
density are
set to '.' meaning that they have no significance as the atoms are dummy 
atoms
included to give the correct composition providing that the
_atom_site_symmetry_multiplicity is given.  The composition defined in the
atom_site loop is linked to the distributed_density loop through the parent-
child identifiers, 'an1' and 'an2'.  The one quarter of the Cp* 
molecules that
are rotating have the occupation number 5/6 x 1/4 = 5/24 = 0.208, the
remainder have the occupation number 5/6 x 3/4 = 15/24 = 0.625.
;
;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_occupancy
  _atom_site_symmetry_multiplicity
  _atom_site_adp_type
  _atom_site_distributed_density_id
  _atom_site_calc_flag
# Inner ring of cyclopentadiene carbon atoms and borazole
C1   C -0.1362(8)  -0.0974(8)  -0.3116(10) 0.0662(18) 0.625(1) 4  Uiso . d
C2   C -0.1060(8)  -0.2165(8)  -0.1837(10) 0.071(2)   0.625(1) 4  Uiso . d
C3   C -0.1774(9)  -0.1939(9)  -0.0820(11) 0.082(2)   0.625(1) 4  Uiso . d
C4   C -0.2529(9)  -0.0561(9)  -0.1479(12) 0.084(2)   0.625(1) 4  Uiso . d
C5   C -0.2261(8)  -0.0002(8)  -0.2891(10) 0.072(2)   0.625(1) 4  Uiso . d
C1a  C   .           .           .          .         0.208(1) 4   .  
an1 dum
C2a  C   .           .           .          .         0.208(1) 4   .  
an1 dum
C3a  C   .           .           .          .         0.208(1) 4   .  
an1 dum
C4a  C   .           .           .          .         0.208(1) 4   .  
an1 dum
C5a  C   .           .           .          .         0.208(1) 4   .  
an1 dum
N1   N -0.1375(8)  -0.0968(8)  -0.3201(10) 0.065(2)   0.167(1) 4   Usso . d
B1   B -0.1002(8)  -0.2265(8)  -0.1728(10) 0.071(2)   0.167(1) 4   Uiso . d
N2   N -0.1402(8)  -0.1034(8)  -0.0765(10) 0.076(2)   0.167(1) 4   Uiso . d
B2   B -0.2370(9)  -0.0364(9)  -0.1832(10) 0.085(2)   0.167(1) 4   Uiso . d
N3   N -0.2893(8)   0.0034(8)  -0.3621(10) 0.062(2)   0.167(1) 4   Uiso . d
B3   B -0.2246(9)  -0.0452(9)  -0.3004(11) 0.073(2)   0.167(1) 4   Uiso . d
# Outer ring of methyl groups
C11  C -0.0951     -0.0733     -0.4330     0.1901     0.625(1) 4   Uani . d
C12  C -0.0272     -0.3236     -0.1750     0.1990     0.625(1) 4   Uani . d
C13  C -0.1719     -0.2833      0.0404     0.2483     0.625(1) 4   Uani . d
C14  C -0.3291     -0.0080     -0.0844     0.2450     0.625(1) 4   Uani . d
C15  C -0.2817      0.1218     -0.3770     0.2219     0.625(1) 4   Uani . d
C11a C   .           .           .          .         0.208(1) 4   .  
an2 dum
C12a C   .           .           .          .         0.208(1) 4   .  
an2 dum
C13a C   .           .           .          .         0.208(1) 4   .  
an2 dum
C14a C   .           .           .          .         0.208(1) 4   .  
an2 dum
C15a C   .           .           .          .         0.208(1) 4   .  
an2 dum
# Details of the two rings of distributed density are given in the following
# loop.
loop_
  _distributed_density_id
  _distributed_density_shape
  _distributed_density_position_x
  _distributed_density_position_y
  _distributed_density_position_z
  _distributed_density_radius
  _distributed_density_direction_h
  _distributed_density_direction_k
  _distributed_density_direction_l
  _distributed_density_Uiso
  _distributed_density_symmetry_multiplicity
an1 ring -0.1810(8)  -0.1133(8)  -0.2058(8)   
                1.198(6)    1.35(2) 0.07(2) -0.45(2)   0.052(2)   4
an2 ring -0.1873(14) -0.1156(14) -0.2210(2)
                2.626(6)    1.30(2) 0.10(2) -0.40(2)   0.131(3)   4
;
#
data_distributed_density_details
    _name             '_distributed_density_details'
    _category          distributed_density
    _type              char
    _list              both
    _list_reference    '_distributed_density_id'
    _example           
;              The distribution was modelled using a disk of scattering
               density of the given radius.
;
    _definition
;              Information about the distribution of scattering density not
               given in other items.
;
#
data_distributed_density_direction_
loop_    _name              
                      '_distributed_density_direction_h'
                      '_distributed_density_direction_k'
                      '_distributed_density_direction_l'
    _category         distributed_density
    _type             numb
    _type_conditions  esd
    _list             both
    _list_reference   '_distributed_density_id'
    _units            rlu
    _units_detail     reciprocal lattice units
    _example          ?
    _definition
             The direction ratios (in reciprocal lattice units) of the 
line of
             distributed density or of the axis of the cylindrical shell or
             ring of distributed density. 
             Note that in a non-orthogonal coordinate system the direction
             ratios of a line are expressed in terms of the reciprocal
             rather than the real lattice.
;
#
data__distributed_density_id
    _name             '_distributed_density_id'
    _category         distributed_density
    _type             char 
    _list             both
    _list_reference   '_distributed_density_id'
    _list_mandatory   yes
    _link_child       '_atom_site_distributed_density_id'
    _example          ?
    _definition       An identifier that links the atom defined by
                      _atom_site_label with a distributed density defined in
                      the distributed_density category.        
;
#
data__distributed_density_length
    _name             '_distributed_density_length'
    _category         distributed_density
    _type             numb
    _type_conditions  esd
    _list             both
    _list_reference   '_distributed_density_id'
    _enumeration_range 0.0:
    _units            A
    _units_detail     Angstrom units
    _example          ?
    _definition
;              The length of the line or cylinder of distributed density in
               Angstrom units.  If this number is set to the translation
               repeat in the direction of the axis of the distribution,
               it describes an infinite line or cylinder of scattering
               density running through the crystal.
;
#
data__distributed_density_position_
loop_    _name              
                      '_distributed_density_position_x'
                      '_distributed_density_position_y'
                      '_distributed_density_position_z'
    _category         distributed_density
    _type             numb
    _type_conditions  esd
    _list             both
    _list_reference   '_distributed_density_id'
    _example          ?
    _definition
;              The position of the centroid of the distributed density in
               fractions of the unit cell values.
;
#
#
data__distributed_density_radius
    _name             '_distributed_density_radius'
    _category         distributed_density
    _type             numb
    _type_conditions  esd
    _list             both
    _list_reference   '_distributed_density_id'
    _enumeration_range 0.0:
    _units            A
    _units_detail     Angstrom units
    _example          ?
    _definition
;              The radius of the cylindrical or spherical shell, or the 
radius
               of the ring of distributed density in Angstrom units.
;
#
data__distributed_density_shape
    _name             '_distributed_density_shape'
    _category         'distributed_density
    _type             char
    _list             both
    _list_reference   '_distributed_density_id'
loop_   
    _enumeration
    _enumeration_detals line       ?
                        ring       ?
                        cylinder   ?
                        sphere     ?
                        other 'Give details in _distributed_density_details'
    _definition
;              A flag that indicates the type of distributed density.  The
               line and ring are one dimensional arrangements of charge and
               the cylinder and sphere are two dimensional charge 
shells.  In
               each case the thickness of the distribution is determined by
               the scattering factor of the element and the atomic
               displacement parameter defined in _distributed_density_Uiso.
;
#
data__distributed_density_symmetry_multiplicity
    _name             '_distributed_density_symmetry_multiplicity'
    _category         distributed_density  
    _type             numb
    _list             both
    _list_reference   '_distributed_density_id'
    _enumeration_range 1:192
    _example          ?
    _definition
;              The number of images of centroid of the distributed density
               that the space group symmetry generates in the unit cell
               reported in the cell category.  It is the number that
               appears in International Tables for Crystallography Vol A for
               the Wyckoff position occupied by the centroid.  Note that all
               the atoms that give rise to the distributed density should be
               listed in the atom_site category even if they, or the 
centroid
               of the distribution, lie on special positions of high 
symmetry.
;
#
data__distributed_density_Uiso
    _name             '_distributed_density_Uiso'
    _category         distributed_density       
    _type             numb
    _type_conditions  esd
    _list             both
    _list_reference   '_distributed_density_id'
    _enumeration_range  0.0:
    _units            A^2^
    _units_detail     'Angstrom units squared'
    _example          0.018(3)
    _definition
;              The value of the isotropic atomic displacement parameter
               applied to each portion of the distributed density.  This
               parameter together with the scattering factor of the atoms
               whose density is distributed, indicates the thickness of the
               line, ring or shell of density.
;
# STATUS: Open for discussion



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