[81bb668] | 1 | r""" |
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| 2 | An alternative version of $P(q)$ for the core-shell ellipsoid |
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| 3 | (see CoreShellEllipsoidModel), having as parameters the core axial ratio X |
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| 4 | and a shell thickness, which are more often what we would like to determine. |
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| 5 | |
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| 6 | This model is also better behaved when polydispersity is applied than the four |
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| 7 | independent radii in CoreShellEllipsoidModel. |
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| 8 | |
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| 9 | Definition |
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| 10 | ---------- |
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| 11 | |
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| 12 | .. figure:: img/core_shell_ellipsoid_fig1.gif |
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| 13 | |
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| 14 | |
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| 15 | The geometric parameters of this model are |
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| 16 | |
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| 17 | *equat_core =* equatorial core radius *= R_minor_core* |
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| 18 | |
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| 19 | *X_core = polar_core / equat_core = Rmajor_core / Rminor_core* |
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| 20 | |
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| 21 | *T_shell = equat_outer - equat_core = Rminor_outer - Rminor_core* |
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| 22 | |
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| 23 | *XpolarShell = Tpolar_shell / T_shell = (Rmajor_outer - Rmajor_core)/ |
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| 24 | (Rminor_outer - Rminor_core)* |
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| 25 | |
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| 26 | In terms of the original radii |
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| 27 | |
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| 28 | *polar_core = equat_core * X_core* |
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| 29 | |
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| 30 | *equat_shell = equat_core + T_shell* |
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| 31 | |
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| 32 | *polar_shell = equat_core * X_core + T_shell * XpolarShell* |
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| 33 | |
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| 34 | (where we note that "shell" perhaps confusingly, relates to the outer radius) |
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| 35 | When *X_core < 1* the core is oblate; when *X_core > 1* it is prolate. |
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| 36 | *X_core = 1* is a spherical core. |
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| 37 | |
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| 38 | For a fixed shell thickness *XpolarShell = 1*, to scale the shell thickness |
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| 39 | pro-rata with the radius *XpolarShell = X_core*. |
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| 40 | |
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| 41 | When including an $S(q)$, the radius in $S(q)$ is calculated to be that of |
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| 42 | a sphere with the same 2nd virial coefficient of the outer surface of the |
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| 43 | ellipsoid. This may have some undesirable effects if the aspect ratio of the |
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| 44 | ellipsoid is large (ie, if $X << 1$ or $X >> 1$ ), when the $S(q)$ |
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| 45 | - which assumes spheres - will not in any case be valid. |
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| 46 | |
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| 47 | If SAS data are in absolute units, and the SLDs are correct, then scale should |
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| 48 | be the total volume fraction of the "outer particle". When $S(q)$ is introduced |
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| 49 | this moves to the $S(q)$ volume fraction, and scale should then be 1.0, |
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| 50 | or contain some other units conversion factor (for example, if you have SAXS data). |
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| 51 | |
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| 52 | References |
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| 53 | ---------- |
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| 54 | |
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| 55 | R K Heenan, *Private communication* |
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| 56 | |
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| 57 | """ |
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| 58 | |
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| 59 | from numpy import inf, sin, cos, pi |
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| 60 | |
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| 61 | name = "core_shell_ellipsoid_xt" |
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| 62 | title = "Form factor for an spheroid ellipsoid particle with a core shell structure." |
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| 63 | description = """ |
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| 64 | [core_shell_ellipsoid_xt] Calculates the form factor for an spheroid |
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| 65 | ellipsoid particle with a core_shell structure. |
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| 66 | The form factor is averaged over all possible |
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| 67 | orientations of the ellipsoid such that P(q) |
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| 68 | = scale*<f^2>/Vol + bkg, where f is the |
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| 69 | single particle scattering amplitude. |
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| 70 | [Parameters]: |
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| 71 | equat_core = equatorial radius of core, |
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| 72 | x_core = polar radius of core, |
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| 73 | t_shell = equatorial radius of outer surface, |
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| 74 | x_polar_shell = polar radius (revolution axis) of outer surface |
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| 75 | core_sld = SLD_core |
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| 76 | shell_sld = SLD_shell |
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| 77 | solvent_sld = SLD_solvent |
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| 78 | background = Incoherent bkg |
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| 79 | scale =scale |
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| 80 | Note:It is the users' responsibility to ensure |
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| 81 | that shell radii are larger than core radii. |
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| 82 | oblate: polar radius < equatorial radius |
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| 83 | prolate : polar radius > equatorial radius - this new model will make this easier |
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| 84 | and polydispersity integrals more logical (as previously the shell could disappear). |
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| 85 | """ |
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| 86 | category = "shape:ellipsoid" |
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| 87 | |
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| 88 | # pylint: disable=bad-whitespace, line-too-long |
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| 89 | # ["name", "units", default, [lower, upper], "type", "description"], |
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| 90 | parameters = [ |
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| 91 | ["equat_core", "Ang", 20, [0, inf], "volume", "Equatorial radius of core"], |
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| 92 | ["x_core", "None", 3, [0, inf], "volume", "Polar radius of core"], |
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| 93 | ["t_shell", "Ang", 30, [0, inf], "volume", "Equatorial radius of shell"], |
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| 94 | ["x_polar_shell", "", 1, [0, inf], "volume", "Polar radius of shell"], |
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| 95 | ["core_sld", "1e-6/Ang^2", 2, [-inf, inf], "", "Core scattering length density"], |
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| 96 | ["shell_sld", "1e-6/Ang^2", 1, [-inf, inf], "", "Shell scattering length density"], |
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| 97 | ["solvent_sld", "1e-6/Ang^2", 6.3, [-inf, inf], "", "Solvent scattering length density"], |
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| 98 | ["theta", "degrees", 0, [-inf, inf], "orientation", "Oblate orientation wrt incoming beam"], |
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| 99 | ["phi", "degrees", 0, [-inf, inf], "orientation", "Oblate orientation in the plane of the detector"], |
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| 100 | ] |
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| 101 | # pylint: enable=bad-whitespace, line-too-long |
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| 102 | |
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| 103 | source = ["lib/gfn.c", "lib/gauss76.c", "core_shell_ellipsoid_xt.c"] |
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| 104 | |
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| 105 | demo = dict(scale=0.05, background=0.001, |
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| 106 | equat_core=20.0, |
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| 107 | x_core=3.0, |
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| 108 | t_shell=30.0, |
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| 109 | x_polar_shell=1.0, |
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| 110 | core_sld=2.0, |
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| 111 | shell_sld=1.0, |
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| 112 | solvent_sld=6.3, |
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| 113 | theta=0, |
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| 114 | phi=0) |
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| 115 | |
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| 116 | oldname = 'CoreShellEllipsoidXTModel' |
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| 117 | |
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| 118 | oldpars = dict(x_polar_shell='XpolarShell', |
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| 119 | x_core='X_core', |
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| 120 | t_shell='T_shell', |
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| 121 | core_sld='sld_core', |
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| 122 | shell_sld='sld_shell', |
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| 123 | solvent_sld='sld_solvent', |
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| 124 | theta='axis_theta', |
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| 125 | phi='axis_phi') |
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| 126 | |
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| 127 | q = 0.1 |
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| 128 | phi = pi/6 |
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| 129 | qx = q*cos(phi) |
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| 130 | qy = q*sin(phi) |
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| 131 | |
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| 132 | tests = [ |
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| 133 | # Accuracy tests based on content in test/utest_coreshellellipsoidXTmodel.py |
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| 134 | [{'equat_core': 200.0, |
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| 135 | 'x_core': 0.1, |
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| 136 | 't_shell': 50.0, |
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| 137 | 'x_polar_shell': 0.2, |
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| 138 | 'core_sld': 2.0, |
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| 139 | 'shell_sld': 1.0, |
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| 140 | 'solvent_sld': 6.3, |
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| 141 | 'background': 0.001, |
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| 142 | 'scale': 1.0, |
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| 143 | }, 1.0, 0.00189402], |
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| 144 | |
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| 145 | # Additional tests with larger range of parameters |
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| 146 | [{'background': 0.01}, 0.1, 11.6915], |
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| 147 | |
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| 148 | [{'equat_core': 20.0, |
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| 149 | 'x_core': 200.0, |
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| 150 | 't_shell': 54.0, |
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| 151 | 'x_polar_shell': 3.0, |
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| 152 | 'core_sld': 20.0, |
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| 153 | 'shell_sld': 10.0, |
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| 154 | 'solvent_sld': 6.0, |
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| 155 | 'background': 0.0, |
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| 156 | 'scale': 1.0, |
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| 157 | }, 0.01, 8688.53], |
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| 158 | |
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| 159 | [{'background': 0.001}, (0.4, 0.5), 0.00690673], |
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| 160 | |
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| 161 | [{'equat_core': 20.0, |
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| 162 | 'x_core': 200.0, |
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| 163 | 't_shell': 54.0, |
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| 164 | 'x_polar_shell': 3.0, |
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| 165 | 'core_sld': 20.0, |
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| 166 | 'shell_sld': 10.0, |
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| 167 | 'solvent_sld': 6.0, |
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| 168 | 'background': 0.01, |
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| 169 | 'scale': 0.01, |
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| 170 | }, (qx, qy), 0.0100002], |
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| 171 | ] |
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