"숫자 163"의 두 판 사이의 차이
21번째 줄: | 21번째 줄: | ||
<h5>j-invariant</h5> | <h5>j-invariant</h5> | ||
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+ | <math>j(\tau)= {E_4(\tau)^3\over \Delta(\tau)}= q^{-1}+744+196884q+21493760q^2+\cdots</math> | ||
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+ | <math>j(\tau)=1728\frac{g_2^3}{g_2^3-27g_3^2}</math> | ||
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+ | <math> E_4(\tau)=1+240\sum_{n>0}\sigma_3(n)q^n= 1+240q+2160q^2+\cdots</math> | ||
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+ | <math>(\sigma_3(n)=\sum_{d|n}d^3)</math> | ||
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+ | <math>\Delta(\tau)= q\prod_{n>0}(1-q^n)^{24}= q-24q+252q^2+\cdots</math> | ||
<math>j(\tau) = \frac{1}{{q}} + 744 + 196884{q} + 21493760{q}^2 + 864299970{q}^3 + \cdots</math><br> 이 때, <math>{q} = e^{2\pi i\tau}</math> | <math>j(\tau) = \frac{1}{{q}} + 744 + 196884{q} + 21493760{q}^2 + 864299970{q}^3 + \cdots</math><br> 이 때, <math>{q} = e^{2\pi i\tau}</math> | ||
40번째 줄: | 52번째 줄: | ||
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66번째 줄: | 78번째 줄: | ||
* Ramanujan observed that <math>\large e^{\pi \sqrt{163}}=262537412640768743.99999999999925\cdots</math> is within <math>10^{-12}</math> of an integer and used this to obtain approximations to <math>\pi</math>. In his Field’s Medal lecture, Richard Borcherds said that every mathematician should see once in his/her life why this should be the case, and this essay is an attempt to do just that. | * Ramanujan observed that <math>\large e^{\pi \sqrt{163}}=262537412640768743.99999999999925\cdots</math> is within <math>10^{-12}</math> of an integer and used this to obtain approximations to <math>\pi</math>. In his Field’s Medal lecture, Richard Borcherds said that every mathematician should see once in his/her life why this should be the case, and this essay is an attempt to do just that. | ||
− | * | + | * <math>640320^3= 262537412640768744</math> |
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<h5>관련된 단원</h5> | <h5>관련된 단원</h5> |
2009년 10월 24일 (토) 00:48 판
간단한 소개
- \(\large e^{\pi \sqrt{163}}=262537412640768743.9999999999992500725\cdots\approx 262537412640768744\)
- \(e^{\pi \sqrt{43}} = 884736743.9997774660349066619374620785\approx 884736744\)
- \(e^{\pi \sqrt{67}} = 147197952743.9999986624542245068292613\approx 147197952744\)
셋 모두 끝 세 자리가 744
complex multiplication
j-invariant
\(j(\tau)= {E_4(\tau)^3\over \Delta(\tau)}= q^{-1}+744+196884q+21493760q^2+\cdots\)
\(j(\tau)=1728\frac{g_2^3}{g_2^3-27g_3^2}\)
\( E_4(\tau)=1+240\sum_{n>0}\sigma_3(n)q^n= 1+240q+2160q^2+\cdots\)
\((\sigma_3(n)=\sum_{d|n}d^3)\)
\(\Delta(\tau)= q\prod_{n>0}(1-q^n)^{24}= q-24q+252q^2+\cdots\)
\(j(\tau) = \frac{1}[[:틀:Q]] + 744 + 196884{q} + 21493760{q}^2 + 864299970{q}^3 + \cdots\)
이 때, \({q} = e^{2\pi i\tau}\)
\( j(\tau)= {E_4(\tau)^3\over \Delta(\tau)}= q^{-1}+744+196884q+21493760q^2+\cdots\)
\( E_4(\tau)=1+240\sum_{n>0}\sigma_3(n)q^n= 1+240q+2160q^2+\cdots\)
\((\sigma_3(n)=\sum_{d|n}d^3)\)
\(\Delta(\tau)= q\prod_{n>0}(1-q^n)^{24}= q-24q+252q^2+\cdots\)
하위주제들
하위페이지
재미있는 사실
- Ramanujan observed that \(\large e^{\pi \sqrt{163}}=262537412640768743.99999999999925\cdots\) is within \(10^{-12}\) of an integer and used this to obtain approximations to \(\pi\). In his Field’s Medal lecture, Richard Borcherds said that every mathematician should see once in his/her life why this should be the case, and this essay is an attempt to do just that.
- \(640320^3= 262537412640768744\)
관련된 단원
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참고할만한 자료
- The Ramanujan Constant. An Essay on Elliptic Curves, Complex. Multiplication and Modular Forms.
- B.J.Green
- http://ko.wikipedia.org/wiki/히그너_수
- http://en.wikipedia.org/wiki/Heegner_number
- http://front.math.ucdavis.edu/search?a=&t=&c=&n=40&s=Listings&q=
- http://www.ams.org/mathscinet/search/publications.html?pg4=AUCN&s4=&co4=AND&pg5=TI&s5=&co5=AND&pg6=PC&s6=&co6=AND&pg7=ALLF&co7=AND&Submit=Search&dr=all&yrop=eq&arg3=&yearRangeFirst=&yearRangeSecond=&pg8=ET&s8=All&s7=
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