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authorSimon Rochester <simon.rochester@gmail.com>2012-10-21 23:08:16 -0700
committerSimon Rochester <simon.rochester@gmail.com>2012-10-21 23:08:16 -0700
commit9a8ad258a0629b391d8239edf1a8e272039b5c93 (patch)
tree1f05b1c17ad29669292638c7ee0f855628de1a41
parent528e6c1576df48bee319baa382f138b46f8314f2 (diff)
downloadNresonances-9a8ad258a0629b391d8239edf1a8e272039b5c93.tar.gz
Nresonances-9a8ad258a0629b391d8239edf1a8e272039b5c93.zip
Allow arbitrary B-field direction.
-rw-r--r--mathemathica_fwm/RbXMDSSetup1.nb523
1 files changed, 183 insertions, 340 deletions
diff --git a/mathemathica_fwm/RbXMDSSetup1.nb b/mathemathica_fwm/RbXMDSSetup1.nb
index 6733d40..9234a7b 100644
--- a/mathemathica_fwm/RbXMDSSetup1.nb
+++ b/mathemathica_fwm/RbXMDSSetup1.nb
@@ -162,26 +162,22 @@ Cell[TextData[{
". Each field can have arbitrary ",
Cell[BoxData[
FormBox[
- SuperscriptBox["\[Sigma]", "+"], TraditionalForm]],
- FormatType->"TraditionalForm"],
+ SuperscriptBox["\[Sigma]", "+"], TraditionalForm]]],
" and ",
Cell[BoxData[
FormBox[
- SuperscriptBox["\[Sigma]", "-"], TraditionalForm]],
- FormatType->"TraditionalForm"],
+ SuperscriptBox["\[Sigma]", "-"], TraditionalForm]]],
" components, labeled ",
Cell[BoxData[
FormBox[
SubscriptBox["\[CapitalOmega]",
- RowBox[{"i", ",", "1"}]], TraditionalForm]],
- FormatType->"TraditionalForm"],
+ RowBox[{"i", ",", "1"}]], TraditionalForm]]],
"and ",
Cell[BoxData[
FormBox[
SubscriptBox["\[CapitalOmega]",
RowBox[{"i", ",",
- RowBox[{"-", "1"}]}]], TraditionalForm]],
- FormatType->"TraditionalForm"],
+ RowBox[{"-", "1"}]}]], TraditionalForm]]],
"."
}], "Text",
CellID->133602844],
@@ -242,8 +238,7 @@ Cell[BoxData[
RowBox[{"(",
RowBox[{
RowBox[{"z", " ",
- SubscriptBox["k", "i"]}], "+",
- SubscriptBox["\[Phi]", "i"], "-",
+ SubscriptBox["k", "i"]}], "-",
RowBox[{"t", " ",
SubscriptBox["\[Omega]", "i"]}]}], ")"}]}]],
RowBox[{"rmes", "\[LeftDoubleBracket]", "i", "\[RightDoubleBracket]"}]],
@@ -251,13 +246,22 @@ Cell[BoxData[
RowBox[{"{",
RowBox[{
RowBox[{"{",
- SubscriptBox["\[CapitalOmega]",
- RowBox[{"i", ",", "1"}]], "}"}], ",",
+ RowBox[{
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+ RowBox[{"\[ImaginaryI]", " ",
+ SubscriptBox["\[Phi]",
+ RowBox[{"i", ",", "p"}]]}]],
+ SubscriptBox["\[CapitalOmega]",
+ RowBox[{"i", ",", "p"}]]}], "}"}], ",",
RowBox[{"{", "0", "}"}], ",",
RowBox[{"{",
- SubscriptBox["\[CapitalOmega]",
- RowBox[{"i", ",",
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+ RowBox[{
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+ RowBox[{"\[ImaginaryI]", " ",
+ SubscriptBox["\[Phi]",
+ RowBox[{"i", ",", "m"}]]}]],
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@@ -284,10 +288,13 @@ Cell[BoxData[
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RowBox[{"ElectricField", "\[Rule]", "field"}], ",",
RowBox[{"MagneticField", "\[Rule]",
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- RowBox[{"0", ",", "0", ",",
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+ RowBox[{
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RowBox[{
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@@ -509,15 +520,7 @@ equivalent to assuming that each field interacts with only the ",
FormBox[
RowBox[{"F", "=", "2"}], TraditionalForm]]],
" ground-state hyperfine sublevel. We also absorb the complex phases into \
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- FormatType->"TraditionalForm"],
- "\[CloseCurlyQuote]s, but the sign of the \[Phi] phase keeps track of the \
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+the \[CapitalOmega]\[CloseCurlyQuote]s."
}], "Text"],
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RowBox[{
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RowBox[{"\[ImaginaryI]", " ",
- SubscriptBox["\[Phi]", "i_"]}]], " ",
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RowBox[{
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RowBox[{
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Cell[TextData[{
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- RowBox[{
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}], "Text"],
-Cell["\<\
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-\>", "Text"],
+Cell["Polarization components for the probe light.", "Text"],
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Relate absorption and phase shift to changes in the real and imaginary parts \
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