PDBx:phasing_MIR_der_reflnType

Data items in the PHASING_MIR_DER_REFLN category record details
about the calculated structure factors obtained in an MIR
phasing experiment.

This list may contain information from a number of different
derivatives; attribute der_id in category phasing_MIR_der_refln indicates to which
 derivative a given record corresponds. (A derivative in this
context does not necessarily equate with a data set; see the
definition of the PHASING_MIR_DER category for a
discussion of the meaning of derivative.)

It is not necessary for the data items describing the measured
value of F to appear in this list, as they will be
given in the PHASING_SET_REFLN category. However, these
items can also be listed here for completeness.

    Example 1 - based on laboratory records for the 6,1,25 reflection
                of an Hg/Pt derivative of protein NS1.
<PDBx:phasing_MIR_der_reflnCategory>
   <PDBx:phasing_MIR_der_refln der_id="HGPT1" index_h="6" index_k="1" index_l="25" set_id="NS1-96">
      <PDBx:F_calc_au>106.66</PDBx:F_calc_au>
      <PDBx:F_meas_au>204.67</PDBx:F_meas_au>
      <PDBx:F_meas_sigma>6.21</PDBx:F_meas_sigma>
      <PDBx:HL_A_iso>-3.15</PDBx:HL_A_iso>
      <PDBx:HL_B_iso>-0.76</PDBx:HL_B_iso>
      <PDBx:HL_C_iso>0.65</PDBx:HL_C_iso>
      <PDBx:HL_D_iso>0.23</PDBx:HL_D_iso>
      <PDBx:phase_calc>194.48</PDBx:phase_calc>
   </PDBx:phasing_MIR_der_refln>
</PDBx:phasing_MIR_der_reflnCategory>

Complex Type Information

Model

Used By

Source

<xsd:complexType name="phasing_MIR_der_reflnType">
  <xsd:annotation>
    <xsd:documentation xml:lang="en">Data items in the PHASING_MIR_DER_REFLN category record details about the calculated structure factors obtained in an MIR phasing experiment. This list may contain information from a number of different derivatives; attribute der_id in category phasing_MIR_der_refln indicates to which derivative a given record corresponds. (A derivative in this context does not necessarily equate with a data set; see the definition of the PHASING_MIR_DER category for a discussion of the meaning of derivative.) It is not necessary for the data items describing the measured value of F to appear in this list, as they will be given in the PHASING_SET_REFLN category. However, these items can also be listed here for completeness. Example 1 - based on laboratory records for the 6,1,25 reflection of an Hg/Pt derivative of protein NS1. <PDBx:phasing_MIR_der_reflnCategory> <PDBx:phasing_MIR_der_refln der_id="HGPT1" index_h="6" index_k="1" index_l="25" set_id="NS1-96"> <PDBx:F_calc_au>106.66</PDBx:F_calc_au> <PDBx:F_meas_au>204.67</PDBx:F_meas_au> <PDBx:F_meas_sigma>6.21</PDBx:F_meas_sigma> <PDBx:HL_A_iso>-3.15</PDBx:HL_A_iso> <PDBx:HL_B_iso>-0.76</PDBx:HL_B_iso> <PDBx:HL_C_iso>0.65</PDBx:HL_C_iso> <PDBx:HL_D_iso>0.23</PDBx:HL_D_iso> <PDBx:phase_calc>194.48</PDBx:phase_calc> </PDBx:phasing_MIR_der_refln> </PDBx:phasing_MIR_der_reflnCategory></xsd:documentation>
  </xsd:annotation>
  <xsd:sequence>
    <xsd:element name="phasing_MIR_der_refln" minOccurs="0" maxOccurs="unbounded">
      <xsd:complexType>
        <xsd:all>
          <xsd:element name="F_calc" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The calculated value of the structure factor for this derivative, in electrons.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="electrons" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="F_calc_au" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The calculated value of the structure factor for this derivative, in arbitrary units.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="arbitrary" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="F_meas" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The measured value of the structure factor for this derivative, in electrons.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="electrons" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="F_meas_au" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The measured value of the structure factor for this derivative, in arbitrary units.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="arbitrary" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="F_meas_sigma" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The standard uncertainty (estimated standard deviation) of attribute F_meas in category phasing_MIR_der_refln, in electrons.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="electrons" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="F_meas_sigma_au" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The standard uncertainty (estimated standard deviation) of attribute F_meas_au in category phasing_MIR_der_refln, in arbitrary units.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="arbitrary" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
          <xsd:element name="HL_A_iso" minOccurs="0" maxOccurs="1" nillable="true" type="xsd:decimal">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The isomorphous Hendrickson-Lattman coefficient A~iso~ for this reflection for this derivative. -2.0 * (Fp~obs~^2^ + Fh~calc~^2^ - Fph~obs~^2^) * Fp~obs~ * cos(alphah~calc~) A~iso~ = ----------------------------------------------- E^2^ E = (Fph~obs~ - Fp~obs~ - Fh~calc~)^2^ for centric reflections = [(Fph~obs~ - Fp~obs~) * 2^1/2^ - Fh~calc~]^2^ for acentric reflections Fp~obs~ = the observed structure-factor amplitude of the native Fph~obs~ = the observed structure-factor amplitude of the derivative Fh~calc~ = the calculated structure-factor amplitude from the heavy-atom model alphah~calc~ = the calculated phase from the heavy-atom model This coefficient appears in the expression for the phase probability of each isomorphous derivative: P~i~(alpha) = exp[k + A * cos(alpha) + B * sin(alpha) + C * cos(2 * alpha) + D * sin(2 * alpha)] Ref: Hendrickson, W. A. & Lattman, E. E. (1970). Acta Cryst. B26, 136-143.</xsd:documentation>
            </xsd:annotation>
          </xsd:element>
          <xsd:element name="HL_B_iso" minOccurs="0" maxOccurs="1" nillable="true" type="xsd:decimal">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The isomorphous Hendrickson-Lattman coefficient B~iso~ for this reflection for this derivative. -2.0 * (Fp~obs~^2^ + Fh~calc~^2^ - Fph~obs~^2^) * Fp~obs~ * sin(alphah~calc~) B~iso~ = ----------------------------------------------- E^2^ E = (Fph~obs~ - Fp~obs~ - Fh~calc~)^2^ for centric reflections = [(Fph~obs~ - Fp~obs~) * 2^1/2^ - Fh~calc~]^2^ for acentric reflections Fp~obs~ = the observed structure-factor amplitude of the native Fph~obs~ = the observed structure-factor amplitude of the derivative Fh~calc~ = the calculated structure-factor amplitude from the heavy-atom model alphah~calc~ = the phase calculated from the heavy-atom model This coefficient appears in the expression for the phase probability of each isomorphous derivative: P~i~(alpha) = exp[k + A * cos(alpha) + B * sin(alpha) + C * cos(2 * alpha) + D * sin(2 * alpha)] Ref: Hendrickson, W. A. & Lattman, E. E. (1970). Acta Cryst. B26, 136-143.</xsd:documentation>
            </xsd:annotation>
          </xsd:element>
          <xsd:element name="HL_C_iso" minOccurs="0" maxOccurs="1" nillable="true" type="xsd:decimal">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The isomorphous Hendrickson-Lattman coefficient C~iso~ for this reflection for this derivative. -Fp~obs~^2^ * [sin(alphah~calc~)^2^ - cos(alphah~calc~)^2^] C~iso~ = ------------------------------------ E^2^ E = (Fph~obs~ - Fp~obs~ - Fh~calc~)^2^ for centric reflections = [(Fph~obs~ - Fp~obs~) * 2^1/2^ - Fh~calc~]^2^ for acentric reflections Fp~obs~ = the observed structure-factor amplitude of the native Fph~obs~ = the observed structure-factor amplitude of the derivative Fh~calc~ = the calculated structure-factor amplitude from the heavy-atom model alphah~calc~ = the phase calculated from the heavy-atom model This coefficient appears in the expression for the phase probability of each isomorphous derivative: P~i~(alpha) = exp[k + A * cos(alpha) + B * sin(alpha) + C * cos(2 * alpha) + D * sin(2 * alpha)] Ref: Hendrickson, W. A. & Lattman, E. E. (1970). Acta Cryst. B26, 136-143.</xsd:documentation>
            </xsd:annotation>
          </xsd:element>
          <xsd:element name="HL_D_iso" minOccurs="0" maxOccurs="1" nillable="true" type="xsd:decimal">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The isomorphous Hendrickson-Lattman coefficient D~iso~ for this reflection for this derivative. -2.0 * Fp~obs~^2^ * sin(alphah~calc~)^2^ * cos(alphah~calc~)^2^ D~iso~ = ---------------------------------------- E^2^ E = (Fph~obs~ - Fp~obs~ - Fh~calc~)^2^ for centric reflections = [(Fph~obs~ - Fp~obs~) * 2^1/2^ - Fh~calc~]^2^ for acentric reflections Fp~obs~ = the observed structure-factor amplitude of the native Fph~obs~ = the observed structure-factor amplitude of the derivative Fh~calc~ = the calculated structure-factor amplitude from the heavy-atom model alphah~calc~ = the phase calculated from the heavy-atom model This coefficient appears in the expression for the phase probability of each isomorphous derivative: P~i~(alpha) = exp[k + A * cos(alpha) + B * sin(alpha) + C * cos(2 * alpha) + D * sin(2 * alpha)] Ref: Hendrickson, W. A. & Lattman, E. E. (1970). Acta Cryst. B26, 136-143.</xsd:documentation>
            </xsd:annotation>
          </xsd:element>
          <xsd:element name="phase_calc" minOccurs="0" maxOccurs="1" nillable="true">
            <xsd:annotation>
              <xsd:documentation xml:lang="en">The calculated value of the structure-factor phase based on the heavy-atom model for this derivative in degrees.</xsd:documentation>
            </xsd:annotation>
            <xsd:complexType>
              <xsd:simpleContent>
                <xsd:extension base="xsd:decimal">
                  <xsd:attribute fixed="degrees" name="units" type="xsd:string" use="optional"/>
                </xsd:extension>
              </xsd:simpleContent>
            </xsd:complexType>
          </xsd:element>
        </xsd:all>
        <xsd:attribute name="der_id" use="required" type="xsd:string">
          <xsd:annotation>
            <xsd:documentation xml:lang="en">This data item is a pointer to attribute id in category phasing_MIR_der in the PHASING_MIR_DER category.</xsd:documentation>
          </xsd:annotation>
        </xsd:attribute>
        <xsd:attribute name="index_h" use="required" type="xsd:integer">
          <xsd:annotation>
            <xsd:documentation xml:lang="en">Miller index h for this reflection for this derivative.</xsd:documentation>
          </xsd:annotation>
        </xsd:attribute>
        <xsd:attribute name="index_k" use="required" type="xsd:integer">
          <xsd:annotation>
            <xsd:documentation xml:lang="en">Miller index k for this reflection for this derivative.</xsd:documentation>
          </xsd:annotation>
        </xsd:attribute>
        <xsd:attribute name="index_l" use="required" type="xsd:integer">
          <xsd:annotation>
            <xsd:documentation xml:lang="en">Miller index l for this reflection for this derivative.</xsd:documentation>
          </xsd:annotation>
        </xsd:attribute>
        <xsd:attribute name="set_id" use="required" type="xsd:string">
          <xsd:annotation>
            <xsd:documentation xml:lang="en">This data item is a pointer to attribute id in category phasing_set in the PHASING_SET category.</xsd:documentation>
          </xsd:annotation>
        </xsd:attribute>
      </xsd:complexType>
    </xsd:element>
  </xsd:sequence>
</xsd:complexType>