§34.2 Definition: 3j Symbol§34.4 Definition: 6j Symbol

§ 34.3. Basic Properties: 3j Symbol

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Contents

§ 34.3(i). Special Cases

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Notes:
See Edmonds (1974, pp. 48–50) and de-Shalit and Talmi (1963, p. 519).
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When any one of j_{{1}},j_{{2}},j_{{3}} is equal to 0,\tfrac{1}{2}, or 1, the 3j symbol has a simple algebraic form. Examples are provided by

34.3.1 \begin{pmatrix}j&j&0\\
m&-m&0\end{pmatrix}=\frac{(-1)^{{j-m}}}{(2j+1)^{{\frac{1}{2}}}},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.2 \begin{pmatrix}j&j&1\\
m&-m&0\end{pmatrix}=(-1)^{{j-m}}\frac{2m}{\left(2j(2j+1)(2j+2)\right)^{{\frac{1}{2}}}}, j\ge\tfrac{1}{2},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.3 \begin{pmatrix}j&j&1\\
m&-m-1&1\end{pmatrix}=(-1)^{{j-m}}\left(\frac{2(j-m)(j+m+1)}{2j(2j+1)(2j+2)}\right)^{{\frac{1}{2}}}, j\ge\tfrac{1}{2}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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For these and other results, and also cases in which any one of j_{1},j_{2},j_{3} is \frac{3}{2} or 2, see Edmonds (1974, pp. 125–127).

Next define

34.3.4 J=j_{1}+j_{2}+j_{3}.
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Defines:
J: sum
Symbols:
j,j_{r}: nonnegative integer
Referenced by:
§34.5(i)
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Then assuming the triangle conditions are satisfied

34.3.5 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
0&0&0\end{pmatrix}=\begin{cases}0,&\mbox{$J$ odd},\\
(-1)^{{\frac{1}{2}J}}\left(\dfrac{(J-2j_{1})!(J-2j_{2})!(J-2j_{3})!}{(J+1)!}\right)^{{\frac{1}{2}}}\dfrac{(\frac{1}{2}J)!}{(\frac{1}{2}J-j_{1})!(\frac{1}{2}J-j_{2})!(\frac{1}{2}J-j_{3})!},&\mbox{$J$ even}.\end{cases}
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol, j,j_{r}: nonnegative integer and J: sum
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Lastly,

34.3.6 \begin{pmatrix}j_{1}&j_{2}&j_{1}+j_{2}\\
m_{1}&m_{2}&-m_{1}-m_{2}\end{pmatrix}=(-1)^{{j_{{1}}-j_{{2}}+m_{{1}}+m_{{2}}}}\left(\frac{(2j_{{1}})!(2j_{{2}})!(j_{{1}}+j_{{2}}+m_{{1}}+m_{{2}})!(j_{{1}}+j_{{2}}-m_{{1}}-m_{{2}})!}{(2j_{{1}}+2j_{{2}}+1)!(j_{{1}}+m_{{1}})!(j_{{1}}-m_{{1}})!(j_{{2}}+m_{{2}})!(j_{{2}}-m_{{2}})!}\right)^{{\frac{1}{2}}},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.7 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
j_{1}&-j_{1}-m_{3}&m_{3}\end{pmatrix}=(-1)^{{-j_{2}+j_{3}+m_{3}}}\left(\frac{(2j_{1})!(-j_{1}+j_{2}+j_{3})!(j_{1}+j_{2}+m_{3})!(j_{3}-m_{3})!}{(j_{1}+j_{2}+j_{3}+1)!(j_{1}-j_{2}+j_{3})!(j_{1}+j_{2}-j_{3})!(-j_{1}+j_{2}-m_{3})!(j_{3}+m_{3})!}\right)^{{\frac{1}{2}}}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(i)
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Again it is assumed that in (34.3.7) the triangle conditions are satisfied.

§ 34.3(ii). Symmetry

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Notes:
See Edmonds (1974, pp. 46–47).
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Even permutations of columns of a 3j symbol leave it unchanged; odd permutations of columns produce a phase factor (-1)^{{j_{{1}}+j_{{2}}+j_{{3}}}}, for example,

34.3.8 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=\begin{pmatrix}j_{2}&j_{3}&j_{1}\\
m_{2}&m_{3}&m_{1}\end{pmatrix}=\begin{pmatrix}j_{3}&j_{1}&j_{2}\\
m_{3}&m_{1}&m_{2}\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(ii)
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34.3.9 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=(-1)^{{j_{{1}}+j_{{2}}+j_{{3}}}}\begin{pmatrix}j_{2}&j_{1}&j_{3}\\
m_{2}&m_{1}&m_{3}\end{pmatrix}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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Next,

34.3.10 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=(-1)^{{j_{{1}}+j_{{2}}+j_{{3}}}}\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
-m_{1}&-m_{2}&-m_{3}\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(ii)
Permalink:
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34.3.11 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=\begin{pmatrix}j_{1}&\frac{1}{2}(j_{{2}}+j_{{3}}+m_{{1}})&\frac{1}{2}(j_{{2}}+j_{{3}}-m_{{1}})\\
j_{{2}}-j_{{3}}&\frac{1}{2}(j_{{3}}-j_{{2}}+m_{{1}})+m_{{2}}&\frac{1}{2}(j_{{3}}-j_{{2}}+m_{{1}})+m_{{3}}\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(ii)
Permalink:
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34.3.12 \begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=\begin{pmatrix}\frac{1}{2}(j_{{1}}+j_{{2}}-m_{{3}})&\frac{1}{2}(j_{{2}}+j_{{3}}-m_{{1}})&\frac{1}{2}(j_{{1}}+j_{{3}}-m_{{2}})\\
j_{{3}}-\frac{1}{2}(j_{{1}}+j_{{2}}+m_{{3}})&j_{{1}}-\frac{1}{2}(j_{{2}}+j_{{3}}+m_{{1}})&j_{{2}}-\frac{1}{2}(j_{{1}}+j_{{3}}+m_{{2}})\end{pmatrix}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(ii)
Permalink:
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Equations (34.3.11) and (34.3.12) are called Regge symmetries. Additional symmetries are obtained by applying (34.3.8)–(34.3.10) to (34.3.11)) and (34.3.12). See Srinivasa Rao and Rajeswari (1993, pp. 44–47) and references given there.

§ 34.3(iii). Recursion Relations

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Notes:
See Edmonds (1974, p. 48).
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In the following three equations it is assumed that the triangle conditions are satisfied by each 3j symbol.

34.3.13 \left((j_{{1}}+j_{{2}}+j_{{3}}+1)(-j_{{1}}+j_{{2}}+j_{{3}})\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=\left((j_{{2}}+m_{{2}})(j_{{3}}-m_{{3}})\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}&j_{{2}}-\frac{1}{2}&j_{{3}}-\frac{1}{2}\\
m_{{1}}&m_{{2}}-\frac{1}{2}&m_{{3}}+\frac{1}{2}\end{pmatrix}-\left((j_{{2}}-m_{{2}})(j_{{3}}+m_{{3}})\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}&j_{{2}}-\frac{1}{2}&j_{{3}}-\frac{1}{2}\\
m_{{1}}&m_{{2}}+\frac{1}{2}&m_{{3}}-\frac{1}{2}\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.14 \left(j_{{1}}(j_{{1}}+1)-j_{{2}}(j_{{2}}+1)-j_{{3}}(j_{{3}}+1)-2m_{{2}}m_{{3}}\right)\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=\left((j_{{2}}-m_{{2}})(j_{{2}}+m_{{2}}+1)(j_{{3}}-m_{{3}}+1)(j_{{3}}+m_{{3}})\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}&j_{{2}}&j_{{3}}\\
m_{{1}}&m_{{2}}+1&m_{{3}}-1\end{pmatrix}+\left((j_{{2}}-m_{{2}}+1)(j_{{2}}+m_{{2}})(j_{{3}}-m_{{3}})(j_{{3}}+m_{{3}}+1)\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}&j_{{2}}&j_{{3}}\\
m_{{1}}&m_{{2}}-1&m_{{3}}+1\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.15 (2j_{{1}}+1)\left((j_{{2}}(j_{{2}}+1)-j_{{3}}(j_{{3}}+1))m_{{1}}-j_{{1}}(j_{{1}}+1)(m_{{3}}-m_{{2}})\right)\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=(j_{{1}}+1)\left(j_{{1}}^{{2}}-(j_{{2}}-j_{{3}})^{{2}}\right)^{{\frac{1}{2}}}\left((j_{{2}}+j_{{3}}+1)^{{2}}-j_{{1}}^{{2}}\right)^{{\frac{1}{2}}}\left(j_{{1}}^{{2}}-m_{{1}}^{{2}}\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}-1&j_{{2}}&j_{{3}}\\
m_{{1}}&m_{{2}}&m_{{3}}\end{pmatrix}+j_{{1}}\left((j_{{1}}+1)^{{2}}-(j_{{2}}-j_{{3}})^{{2}}\right)^{{\frac{1}{2}}}\left((j_{{2}}+j_{{3}}+1)^{{2}}-(j_{{1}}+1)^{{2}}\right)^{{\frac{1}{2}}}\left((j_{{1}}+1)^{{2}}-m_{{1}}^{{2}}\right)^{{\frac{1}{2}}}\begin{pmatrix}j_{{1}}+1&j_{{2}}&j_{{3}}\\
m_{{1}}&m_{{2}}&m_{{3}}\end{pmatrix}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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Encodings:
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For these and other recursion relations see Varshalovich et al. (1988, §8.6). See also Micu (1968), Louck (1958), Schulten and Gordon (1975a), Srinivasa Rao and Rajeswari (1993, pp. 220–225), and Luscombe and Luban (1998).

§ 34.3(iv). Orthogonality

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Notes:
See Edmonds (1974, p. 47), de-Shalit and Talmi (1963, p. 515).
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34.3.16 \sum _{{m_{1}m_{2}}}(2j_{3}+1)\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}\begin{pmatrix}j_{1}&j_{2}&j^{{\prime}}_{3}\\
m_{1}&m_{2}&m^{{\prime}}_{3}\end{pmatrix}=\delta _{{j_{{3}},j^{{\prime}}_{{3}}}}\delta _{{m_{{3}},m^{{\prime}}_{{3}}}},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(iv), §34.9
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34.3.17 \sum _{{j_{{3}}m_{{3}}}}(2j_{{3}}+1)\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m^{{\prime}}_{1}&m^{{\prime}}_{2}&m_{3}\end{pmatrix}=\delta _{{m_{{1}},m^{{\prime}}_{{1}}}}\delta _{{m_{{2}},m^{{\prime}}_{{2}}}},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
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34.3.18 \sum _{{m_{{1}}m_{{2}}m_{{3}}}}\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}=1.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and j,j_{r}: nonnegative integer
Referenced by:
§34.3(iv)
Permalink:
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In the summations (34.3.16) – (34.3.18) the summation variables range over all values that satisfy the conditions given in (34.2.1) – (34.2.3). Similar conventions apply to all subsequent summations in this chapter.

§ 34.3(v). Generating Functions

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For generating functions for the 3j symbol see Biedenharn and van Dam (1965, p. 245, Eq. (3.42) and p. 247, Eq. (3.55)).

§ 34.3(vi). Sums

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For sums of products of 3j symbols, see Varshalovich et al. (1988, pp. 259–262).

§ 34.3(vii). Relations to Legendre Polynomials and Spherical Harmonics

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Notes:
See Thompson (1994, p. 288), Edmonds (1974, p. 63).
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For the polynomials P_{{l}} see §Ch.18, and for the functions Y_{{{l},{m}}} and {Y_{{{l},{m}}}^{{*}}} see §Ch.14.

34.3.19 P_{{l_{1}}}\!\left(\cos\theta\right)P_{{l_{2}}}\!\left(\cos\theta\right)=\sum _{l}(2l+1)\begin{pmatrix}l_{1}&l_{2}&l\\
0&0&0\end{pmatrix}^{2}P_{{l}}\!\left(\cos\theta\right),
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and l,l_{r}: nonnegative integer
Referenced by:
§34.3(vii)
Permalink:
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Encodings:
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34.3.20 Y_{{{l_{1}},{m_{1}}}}\!\left(\theta,\phi\right)Y_{{{l_{2}},{m_{2}}}}\!\left(\theta,\phi\right)=\sum _{{l,m}}\left(\frac{(2l_{1}+1)(2l_{2}+1)(2l+1)}{4\pi}\right)^{{\frac{1}{2}}}\begin{pmatrix}l_{1}&l_{2}&l\\
m_{1}&m_{2}&m\end{pmatrix}{Y_{{{l},{m}}}^{{*}}}\!\left(\theta,\phi\right)\begin{pmatrix}l_{1}&l_{2}&l\\
0&0&0\end{pmatrix},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and l,l_{r}: nonnegative integer
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Encodings:
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34.3.21 \int _{0}^{\pi}P_{{l_{1}}}\!\left(\cos\theta\right)P_{{l_{2}}}\!\left(\cos\theta\right)P_{{l_{3}}}\!\left(\cos\theta\right)\sin\theta d\theta=2\begin{pmatrix}l_{1}&l_{2}&l_{3}\\
0&0&0\end{pmatrix}^{2},
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and l,l_{r}: nonnegative integer
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Encodings:
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34.3.22 \int _{0}^{{2\pi}}\!\int _{0}^{{\pi}}Y_{{{l_{1}},{m_{1}}}}\!\left(\theta,\phi\right)Y_{{{l_{2}},{m_{2}}}}\!\left(\theta,\phi\right)Y_{{{l_{3}},{m_{3}}}}\!\left(\theta,\phi\right)\sin\theta d\theta d\phi=\left(\frac{(2l_{1}+1)(2l_{2}+1)(2l_{3}+1)}{4\pi}\right)^{{\frac{1}{2}}}\begin{pmatrix}l_{1}&l_{2}&l_{3}\\
0&0&0\end{pmatrix}\begin{pmatrix}l_{1}&l_{2}&l_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}.
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Symbols:
\begin{pmatrix}j_{1}&j_{2}&j_{3}\\
m_{1}&m_{2}&m_{3}\end{pmatrix}: 3j symbol and l,l_{r}: nonnegative integer
Referenced by:
§34.3(vii)
Permalink:
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Encodings:
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Equations (34.3.19) – (34.3.22) are particular cases of more general results that relate rotation matrices to 3j symbols, for which see Edmonds (1974, Chapter 4). The left- and right-hand sides of (34.3.22) are known, respectively, as Gaunt's integral and the Gaunt coefficient (Gaunt (1929)).