MCP๋กœ ์—ฐ๊ฒฐ โ†’

๊ณ„์‚ฐ ์ž…๋ ฅ

x โ‰ค 0์ธ ๊ฒฝ์šฐ ์‹ค์ˆ˜๊ฐ’ ๊ฒฐ๊ณผ๊ฐ€ ๋ณต์†Œ์ˆ˜๊ฐ€ ๋˜๊ฑฐ๋‚˜ ์ •์˜๋˜์ง€ ์•Š์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค.

๊ณต์‹

Show calculation steps (2)
  1. Upward recurrence to order v

    Upward recurrence to order v: ๋ณ€ํ˜• ๊ตฌ๋ฉด ๋ฒ ์…€ ํ•จ์ˆ˜ i_v(x), k_v(x) ๋ฐ ๋„ํ•จ์ˆ˜ ๊ณ„์‚ฐ๊ธฐ

    Applied for v = Order >= 1 to reach i_v and k_v; n runs from 1 up to v.

  2. Derivatives

    Derivatives: ๋ณ€ํ˜• ๊ตฌ๋ฉด ๋ฒ ์…€ ํ•จ์ˆ˜ i_v(x), k_v(x) ๋ฐ ๋„ํ•จ์ˆ˜ ๊ณ„์‚ฐ๊ธฐ

    First derivatives of the modified spherical Bessel functions at order v.

๊ด‘๊ณ 

๊ฒฐ๊ณผ

Modified Spherical Bessel (first kind) iv(x)
1.8134302039
๋ฌด์ฐจ์›
Second kind kv(x) 0.1062920829
Derivative i'v(x) -0.9743827436
Derivative k'v(x) -0.1594381243

์ด ๊ณ„์‚ฐ๊ธฐ์˜ ๊ธฐ๋Šฅ

์ด ๋„๊ตฌ๋Š” ์Œ์ด ์•„๋‹Œ ์ •์ˆ˜ ์ฐจ์ˆ˜ v์™€ ์–‘์˜ ์‹ค์ˆ˜ ์ธ์ž x์— ๋Œ€ํ•ด ๋ณ€ํ˜• ๊ตฌ๋ฉด ๋ฒ ์…€ ํ•จ์ˆ˜ ์ œ1์ข… \(i_v(x)\), ์ œ2์ข… \(k_v(x)\)์™€ ํ•จ๊ป˜ 1์ฐจ ๋„ํ•จ์ˆ˜ \(i'_v(x)\), \(k'_v(x)\)๋ฅผ ๊ณ„์‚ฐํ•ฉ๋‹ˆ๋‹ค. ์ด๋“ค์€ ์ˆœ์ˆ˜ํ•œ ์ˆ˜ํ•™์  ํŠน์ˆ˜ํ•จ์ˆ˜๋กœ, ์ง€์—ญ์ด๋‚˜ ๋‹จ์œ„์— ๊ด€ํ•œ ์–ด๋– ํ•œ ๊ฐ€์ •๋„ ์—†์ด ์–ด๋””์„œ๋‚˜ ๋™์ผํ•˜๊ฒŒ ์ ์šฉ๋ฉ๋‹ˆ๋‹ค.

๋ฐฐ๊ฒฝ ์ง€์‹๊ณผ ๊ณต์‹

์ด ํ•จ์ˆ˜๋“ค์€ ๋ณ€ํ˜• ๊ตฌ๋ฉด ๋ฒ ์…€ ๋ฐฉ์ •์‹ \(x^2 w'' + 2x w' - (x^2 + v(v+1))w = 0\)์˜ ํ•ด์ž…๋‹ˆ๋‹ค. ๋ฐ˜์ •์ˆ˜ ์ฐจ์ˆ˜ ์ด๋™์„ ํ†ตํ•ด ์›ํ†ตํ˜• ๋ณ€ํ˜• ๋ฒ ์…€ ํ•จ์ˆ˜์™€ ๋‹ค์Œ๊ณผ ๊ฐ™์ด ์—ฐ๊ฒฐ๋ฉ๋‹ˆ๋‹ค.

$$i_v(x) = \sqrt{\frac{\pi}{2x}}\,I_{v+1/2}(x), \qquad k_v(x) = \sqrt{\frac{2}{\pi x}}\,K_{v+1/2}(x)$$

์ •์ˆ˜ v์— ๋Œ€ํ•ด +1/2 ์ด๋™์œผ๋กœ ์ฐจ์ˆ˜๊ฐ€ ๋ฐ˜์ •์ˆ˜๊ฐ€ ๋˜๋ฏ€๋กœ, ์ด ํ•จ์ˆ˜๋“ค์€ sinh, cosh, exp๋กœ ์ด๋ฃจ์–ด์ง„ ์ดˆ๋“ฑํ•จ์ˆ˜ ํ‘œํ˜„์œผ๋กœ ํ™˜์›๋ฉ๋‹ˆ๋‹ค. ์ดˆ๊ธฐ๊ฐ’์œผ๋กœ

$$i_0 = \frac{\sinh x}{x}, \quad i_1 = \frac{\cosh x}{x} - \frac{\sinh x}{x^{2}}$$$$k_0 = \frac{\pi}{2x}\,e^{-x}, \quad k_1 = \frac{\pi}{2x}\,e^{-x}\!\left(1 + \frac{1}{x}\right)$$

๋ฅผ ์‚ฌ์šฉํ•œ ๋’ค, ์›ํ•˜๋Š” ์ฐจ์ˆ˜๊นŒ์ง€ ์œ„๋กœ ์ ํ™”์‹œํ‚ต๋‹ˆ๋‹ค. ๋„ํ•จ์ˆ˜๋Š” \(f'_v = -f_{v+1} + \frac{v}{x}f_v\)๋กœ ๊ตฌํ•ฉ๋‹ˆ๋‹ค.

x๊ฐ€ ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ๋ณ€ํ˜• ๊ตฌ๋ฉด ๋ฒ ์…€ ํ•จ์ˆ˜ i๋Š” ์ฆ๊ฐ€ํ•˜๊ณ  k๋Š” ๊ฐ์†Œํ•˜๋Š” ๊ทธ๋ž˜ํ”„
x๊ฐ€ ์ฆ๊ฐ€ํ•˜๋ฉด ์ œ1์ข… ํ•จ์ˆ˜ i_v(x)๋Š” ์ฆ๊ฐ€ํ•˜๊ณ  k_v(x)๋Š” ๊ฐ์†Œํ•ฉ๋‹ˆ๋‹ค.

์‚ฌ์šฉ ๋ฐฉ๋ฒ•

์ •์ˆ˜ ์ฐจ์ˆ˜ v(0, 1, 2, โ€ฆ)์™€ \(x > 0\)์ธ ์ธ์ž x๋ฅผ ์ž…๋ ฅํ•œ ๋’ค ๋„ค ๊ฐ€์ง€ ๊ฒฐ๊ณผ๊ฐ’์„ ํ™•์ธํ•˜์„ธ์š”. ์—ฌ๊ธฐ์„œ๋Š” \(k_v(x) = \sqrt{\frac{2}{\pi x}}\,K_{v+1/2}(x)\) ๊ทœ์•ฝ์„ ์‚ฌ์šฉํ•˜๋ฉฐ, ์ด๋กœ ์ธํ•ด \(k_0\)์— ๋ณด์ด๋Š” \(\pi/2\) ์ธ์ž๊ฐ€ ์ƒ๊น๋‹ˆ๋‹ค. ์ผ๋ถ€ ๋ฌธํ—Œ์—์„œ๋Š” ์ด ์ธ์ž๋ฅผ ์ƒ๋žตํ•˜๊ธฐ๋„ ํ•ฉ๋‹ˆ๋‹ค.

๊ณ„์‚ฐ ์˜ˆ์‹œ (v = 0, x = 2)

$$i_0(2) = \frac{\sinh(2)}{2} = \frac{3.6268604}{2} = 1.8134302$$$$i_1(2) = \frac{\cosh(2)}{2} - \frac{\sinh(2)}{4} = 1.8810978 - 0.9067151 = 0.9743827$$์ด๋ฏ€๋กœ \(i'_0(2) = -i_1(2) = -0.9743827\).$$k_0(2) = \frac{\pi}{4}e^{-2} = 0.1062930, \qquad k_1(2) = k_0 \cdot 1.5 = 0.1594394$$์ด๋ฏ€๋กœ \(k'_0(2) = -k_1(2) = -0.1594394\).

์ž์ฃผ ๋ฌป๋Š” ์งˆ๋ฌธ

์ •์ˆ˜๊ฐ€ ์•„๋‹Œ ์ฐจ์ˆ˜ v๋ฅผ ์‚ฌ์šฉํ•  ์ˆ˜ ์žˆ๋‚˜์š”? ์ด ์‹ค์ˆ˜๊ฐ’ ์ฝ”๋“œ๋Š” ํ•จ์ˆ˜๊ฐ€ ์ดˆ๋“ฑํ•จ์ˆ˜๊ฐ€ ๋˜๋Š” ์Œ์ด ์•„๋‹Œ ์ •์ˆ˜ ์ฐจ์ˆ˜๋ฅผ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค. ์ •์ˆ˜๊ฐ€ ์•„๋‹Œ ์ฐจ์ˆ˜๋Š” ์™„์ „ํ•œ I/K ๋ฒ ์…€ ํ•จ์ˆ˜ ๊ณ„์‚ฐ์ด ํ•„์š”ํ•ฉ๋‹ˆ๋‹ค.

์™œ x๋Š” ์–‘์ˆ˜์—ฌ์•ผ ํ•˜๋‚˜์š”? \(k_v(x)\)๋Š” \(x \to 0\)์ผ ๋•Œ ๋ฐœ์‚ฐํ•˜๊ณ , \(x < 0\)์ด๋ฉด ๊ฒฐ๊ณผ๊ฐ€ ๋ณต์†Œ์ˆ˜๊ฐ€ ๋˜๋ฏ€๋กœ ์‹ค์ˆ˜ ๋ฒ„์ „์—์„œ๋Š” \(x > 0\)๊ฐ€ ํ•„์š”ํ•ฉ๋‹ˆ๋‹ค.

iv์™€ kv์˜ ์ฐจ์ด๋Š” ๋ฌด์—‡์ธ๊ฐ€์š”? \(i_v\)๋Š” ์ง€์ˆ˜์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜๋ฉฐ ์›์ ์—์„œ ์ •์น™(regular)์ž…๋‹ˆ๋‹ค. ๋ฐ˜๋ฉด \(k_v\)๋Š” ์ง€์ˆ˜์ ์œผ๋กœ ๊ฐ์†Œํ•˜๋ฉฐ ์›์ ์—์„œ ํŠน์ด์ ์„ ๊ฐ€์ง‘๋‹ˆ๋‹ค.

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