• 検索結果がありません。

Lanczos法を利用したTSVD法の積分方程式への応用

N/A
N/A
Protected

Academic year: 2021

シェア "Lanczos法を利用したTSVD法の積分方程式への応用"

Copied!
6
0
0

読み込み中.... (全文を見る)

全文

(1)Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report. Lanczos ๏Λར༻ͨ͠ TSVD ๏ͷੵ෼ํఔࣜ΁ͷԠ༻ ลɹԕ1,a). ໺ࣉɹོ2,b). ֓ཁɿຊߘ͸ɼඇద੾໰୊ͷதͰ୅දతͳୈҰछ Fredholm ੵ෼ํఔࣜͷ਺஋ղ๏ʹ͍ͭͯߟ͑Δɽ࠷ॳ ʹɼ͜ͷΑ͏ͳ໰୊ͷղ๏ʹ༻͍ΒΕΔ TSVD ͷ‫ج‬ຊతͳߟ͑ํʹ͍ͭͯड़΂Δɽ࣍ʹɼTSVD ๏Λ࣮ߦ Ͱ͖Δ‫ݹ‬యతͳ Lanczos ๏ʹ͍ͭͯɼॏΈ෇͖ͷੵ෼ެࣜΛ༻͍ͨ৔߹ʹਫ਼౓ྑۙ͘ࣅղΛ‫͖Ͱࢉܭ‬Δम ਖ਼๏ΛఏҊ͢Δɽ࠷‫ʹޙ‬ɼ਺஋࣮‫ݧ‬Λ௨ͯ͠ɼఏҊख๏ͷ༗ޮੑʹ͍ͭͯड़΂Δɽ. Lanczos type iteration to TSVD method for solving Fredholm integral equation of the first kind Yuan Bian1,a). Takashi Nodera2,b). Abstract: Recently, a method called TSVD (Truncated Singular Value Decomposition) has been attracting some attention for solving Fredholm integral equation of the first kind. Solving a discretized this problem is a well-known ill-conditioned problem. This paper explains why the TSVD method performs well when solving Fredholm integral equations of the first kind, and proposes a new kind of TSVD method, which is combined with the Lanczos method. The results of numerical experiments are shown to confirm the effectiveness of our proposed method.. ͕ඇৗʹେ͖͍ɽͭ·Γɼ‫ࢉܭ‬தͰඍখͳ‫Ͱࠩޡ‬΋݁Ռʹ. 1. ͸͡Ίʹ. ലେͳӨ‫ڹ‬Λ༩͑Δ͜ͱʹͳΔɽΏ͑ʹɼͨͩ x = A−1 b. ୈҰछ Fredholm ੵ෼ํఔࣜ:  b K(x, y)f (y)dy = g(x). Ͱ‫͢ࢉܭ‬Ε͹େ͖ͳ‫͕ࠩޡ‬ੜ͡ΔՄೳੑ͕ߴ͘ɼਫ਼౓ͷΑ ͍ղΛ‫ٻ‬ΊΔͷ͸ͦΕ΄Ͳ༰қͰ͸ͳ͍ɽͦΕղܾࡦͷ 1. (1). a. Λߟ͑Δɽͨͩ͠ɼੵ෼֩ͱ‫ݺ‬͹ΕΔ 2 ม਺ؔ਺ K(x, y) ͱӈଆͷؔ਺ g(x) ͕‫ط‬஌Ͱɼf (y) ͸‫ٻ‬Ί͍ͨະ஌ؔ਺Ͱ ͋Δɽ͜͜Ͱɼf, g ∈ L2 [a, b]ɼK ∈ L2 ([a, b] × [a, b]) Λߟ ͑Δɽ͜ͷํఔࣜΛ཭ࢄԽ͢͠Δͱɼ࣍ͷΑ͏ͳઢ‫ํܗ‬ఔ ͕ಘΒΕΔɽ. Ax = b,. A∈R. , b∈R. n. (2). Ұछ Fredholm ੵ෼ํఔࣜΛ཭ࢄԽͯ͠ಘΒΕΔͷͰ୅ද తͳѱ৚݅໰୊ͱͳΓɼ΄ͱΜͲͷ৔߹Ͱߦྻ A ͷ৚݅਺. 2 a) b). TSVD(Truncated Singular Value Decomposition) ๏͸ɼ ѱ৚݅ͷઢ‫ํܗ‬ఔࣜ (2) Λղͨ͘ΊʹΑ͘࢖ΘΕΔख๏ͷ. 1 ͭͰ͋Δɽಛʹඇద੾ͳ໰୊ͱͯ͠஌ΒΕ͍ͯΔୈҰछ Fredholm ੵ෼ํఔࣜͷ਺஋ղͱͯ͠༗ޮͰ͋Δɽ ߦྻ A ͷ৚݅਺͕ඇৗʹେ͖͍৔߹ɼ௨ৗɼߦྻ A ͕ ଟ਺ͷ 0 ʹ͍ۙಛҟ஋Λ࣋ͭ͜ͱ͕ଟ͍ɽͦͷͨΊɼͦΕ. n×n. ࣜ (2) ͸ɼ਺஋తʹ؆୯ʹղ͚ͦ͏ʹ‫͑ݟ‬Δ͕ɼ࣮ࡍɼୈ. 1. ͭ͸ɼTSVD ๏Λར༻͢Δ͜ͱͰ͋Δɽ. ‫ܚ‬ጯٛक़େֶେֶӃཧ޻ֶ‫ڀݚ‬Պ ˟ 223-8522 ԣ඿ࢢߓ๺۠೔٢ 3-14-1 ‫ܚ‬ጯٛक़େֶཧ޻ֶ෦ ˟ 223-8522 ɹԣ඿ࢢߓ๺۠೔٢ 3-14-1 [email protected] [email protected]. ⓒ 2018 Information Processing Society of Japan. ΒΛ௚઀ 0 ʹ͢Δ͜ͱʹΑΓ ɼ৚݅਺Λஶ͘͠‫ݮ‬গͤ͞ Δ͜ͱ͕Ͱ͖ɼਫ਼౓ͷΑ͍ղΛಘΔ͜ͱ͕‫ظ‬଴Ͱ͖Δͷ͕. TSVD ๏ͷ‫ج‬ຊతͳߟ͑ํͰ͋Δɽ۩ମతʹ‫͑ݴ‬͹ɼߦྻ A ͕࣍ͷΑ͏ͳಛҟ஋෼ղΛ࣋ͭͱ͢Δɽ A = U ΣV ∗ , Σ = diag{σ1 , σ2 , · · · , σn }. (3). ΋͠ σk+1 , · · · , σn ͕ 0 ʹ͍ۙಛҟ஋Ͱ͋Ε͹ɼͦΕΒΛ௚ ઀ 0 ʹ͢Δɽ͜ͷૢ࡞Ͱɼ‫ݩ‬ͷߦྻ A ͕࣍ͷΑ͏ʹͳΔɽ. Ak = U Σk V ∗ , Σk = diag{σ1 , σ2 , · · · , σk 0, · · · , 0} (4) 1.

(2) Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report. ͜͜ͰɼAk ͕ਖ਼ଇߦྻͰͳ͍ͨΊɼਖ਼֬ͳղ͕ඞͣ͠΋ ଘࡏ͢Δͱ͸‫ݶ‬Βͳ͍ɽͦΕ‫ʹނ‬ɼ৽͍͠໰୊Λ࠷খೋ৐ ໰୊ͱͯ͠ղ͘ඞཁ͕͋Δɽ. ui = σi−1 Kvi. (10). ui ͷఆٛΑΓɼ಺ੵ ui , ui  ͱ ui , uj ʢͨͩ͠ɼui = uj ʣ ͸ɼ࣍ͷΑ͏ʹ‫͖Ͱࢉܭ‬Δɽ. xk = argmin Ak x − b. (5). x. ui , ui  = σi−1 Kvi , σi−1 Kvi  = σi−2 vi , K∗ Kvi . ͜ͷ࠷খೋ৐໰୊Λղ͍ͯɼxk ͸࣍ͷࣜͰ༩͑ΒΕΔɽ. xk = V Σ−1 k U∗ b. (6). = σi−2 vi , σi2 vi  = 1 ui , uj  =. ߟ͑ํʹͦͷ··ैͬͯ‫͢ࢉܭ‬Δͱɼߦྻ A ͷ‫׬‬શͳಛҟ ஋෼ղ͕ඞཁͰ͋ΔͨΊɼे෼ͳ‫͕ؒ࣌ࢉܭ‬ඞཁͱͳΔɽ ͦΕ͚ͩͰͳ͘ɼ্‫ه‬ͷٞ࿦͚ͩͰɼxk ͕ x ʹ͍ۙɼଈ ͪɼಛҟ஋ͷ੾Γࣺͯͷૢ࡞͕ղʹ΋ͨΒ͢Ө‫͕ڹ‬খ͍͞. =. σi−2 vi , K∗ Kvj . = σi−2 vi , σi2 vj  = 0. ‫ࢉܭ‬ͷ్தͰখ͍͞ಛҟ஋͕࢖ΘΕͳ͔ͬͨͨΊɼxk Λ ൺֱతਫ਼౓Α͘‫ٻ‬ΊΔ͜ͱ͕Ͱ͖Δɽ͔͠͠ɼTSVD ๏ͷ. (11). σi−1 Kvi , σi−1 Kvj . (12). ࣜ (11) ͱ (12) ΑΓɼ{ui }∞ i=1 ΋ਖ਼‫ن‬௚ަ‫ܥ‬Λͳ͢ɽ ࣍ʹɼK∗ ui Λߟ͑Δɽ. K∗ ui = K∗ σi−1 Kvi  = σi−1 K∗ Kvi  = σvi. (13). ࣜ (10) ͱࣜ (13) Λ߹Θͤͯɼ࣍ͷ͜ͱ͕Θ͔Δɽ. ͜ͱΛઆ໌͢Δͷ͸ࢸ೉ͷٕͰ͋Δɽ ຊߘͰ͸ͦͷΑ͏ͳ໰୊఺Λվળͯ͠ɼ·ͣ࿈ଓͷࢹ఺ ͔ΒɼୈҰछ Fredholm ੵ෼ํఔࣜͷͨΊͷ TSVD ๏Λಋ ग़͠ɼੵ෼ํఔࣜʹର͢Δ༗ޮੑʹ͍ͭͯड़΂Δɽ࣍ʹɼ ཭ࢄԽͨ͠໰୊ʹରͯ͠ɼLanczos ๏Λར༻ͨ͠ TSVD ๏ ΛఏҊ͢Δɽ࠷‫ʹޙ‬ɼ͍͔ͭ͘ͷ਺஋࣮‫ݧ‬Λ௨ͯ͠ɼఏҊ ख๏ͷ༗ޮੑΛ‫͢ূݕ‬Δɽ. Kvi = σi ui , K∗ ui = σi vi. (14). ࣜ (14) ΑΓɼσi ɼui ɼvi ͸ K ʹରͯ͠ɼߦྻͷಛҟ஋ͱಛ ҟϕΫτϧͱࣅͨΑ͏ͳ໾ׂͰ͋ΔɽͦΕΒΛ༻͍ͯɼؔ ਺ K(x, y) ͷߦྻͷಛҟ஋෼ղͱಉ༷ͳ΋ͷΛߟ͑Δɽ. vi ͷ ఆ ٛ Α Γ ɼK(x, y) ͸ vi ͱ ಺ ੵ Λ औ Ε Δ ͜ ͱ ͕ อ ূ ͞ Ε Δ ɽ‫ ʹ ނ‬ɼK(x, y) Λ y ͷ ؔ ਺ ͱ Έ ͳ ͤ ͹ ɼ. 2. ୈҰछ Fredholm ੵ෼ํఔࣜͷ TSVD ๏ ࣜ (1) Ͱ༩͑ΒΕͨੵ෼ํఔࣜΛߟ͑Δɽͦͷੵ෼Λؔ ਺ f ʹֻ͚Δ࡞༻ૉͱΈͳͤ͹ɼ࡞༻ૉͷ‫͖ॻͰࣜܗ‬௚͢. K(x, y) ∈ span{vi }∞ i=1 Ͱ͋ΔɽͦͷͨΊɼK(x, y) ʹର ͯ࣍͠ͷΑ͏ͳల։͕Ͱ͖Δɽ. K(x, y) =. ͜ͱ͕Ͱ͖Δɽ. Kf = g. =. (7). ͜͜Ͱɼ࡞༻ૉ K ͸࣍ͷΑ͏ͳ΋ͷͰ͋Δɽ  b Kf (y) = K(x, y)f (y)dy. =. i=1 ∞  i=1 ∞ . K(x, y), vi (y)vi (y) (Kvi )vi (y) σi ui (x)vi (y). (15). i=1. (8). a. ∞ . ࣜ (15) ΑΓɼߦྻͷಛҟ஋෼ղͱྨࣅ͢Δؔ਺ K(x, y) ͷ. ͨͩ͠ɼK ∈ L2 ([a, b] × [a, b]) ΑΓɼK ͸ L2 [a, b] ͔Β. ಛҟ஋෼ղ͕ಘΒΕͨɽ࣍ʹɼ͜ͷ෼ղΛ༻͍ͯɼ‫ݩ‬ͷํ. L2 [a, b] ΁ͷ࡞༻ૉͰɼ༗քʢΏ͑ʹ࿈ଓʣઢ‫༻࡞ܕ‬ૉͰ͋. ఔࣜͷղΛߟ͑Δɽ. ∗. ΔɽͦͷͨΊɼਵ൐࡞༻ૉ K ͕ଘࡏ͢Δɽ·ͨɼK ͕ί ∗. ϯύΫτͰ͋Δ͜ͱ΋ূ໌Ͱ͖Δ [6]ɽΑͬͯɼK K ͕ࣗ ‫ݾ‬ਵ൐ͳ൒ਖ਼ఆ஋Ͱɼ͔ͭίϯύΫτͳ࡞༻ૉͰ͋Γɼ࣍. i = 1, 2, · · ·. ͏ʹͳΔɽ. . b. K(x, y)f (y)dy =. ࣜΛຬͨ͢‫ݻ‬༗஋ σi ͱ‫ݻ‬༗ؔ਺ vi ͕ଘࡏ͢Δɽ. K∗ Kvi = σi vi ,. ࣜ (15) Λ࠷ॳͷํఔࣜ (1) ʹ୅ೖ͢Δͱɼࠨଆ͕࣍ͷΑ. a. (9). =. ͞Βʹɼ{vi }∞ i=1 ͸ਖ਼‫ن‬௚ަ‫ܥ‬Λͳ͢ɽ·ͨɼඇྵͷ σi ͷ ‫͕਺ݸ‬༗‫ݸݶ‬ɼ·ͨ͸Մࢉແ‫͋Ͱݸݶ‬Δ [5]ɽͦ͜Ͱɼ࠷. =. i=1 ∞  i=1 ∞ . b a. σi ui (x)vi (y)f (y)dy. σi ui (x). . b a. vi (y)f (y)dy. σi f, vi ui (x). (16). i=1. ॳʹɼඇྵͷ σi ͷ‫͕਺ݸ‬Մࢉແ‫͋Ͱݸݶ‬ΔͷΛԾఆ͢Δɽ ༗‫ݸݶ‬ͷ৔߹͸ຊઅͷ࠷‫͑ߟͰޙ‬Δ͜ͱʹ͢Δɽ. ∞  . ࣜ (16) ΑΓɼࣜ (1) ͷࠨଆ͕ਖ਼‫ن‬௚ަ‫{ ܥ‬ui }∞ i=1 ͷுΔۭ ؒʹೖ͍ͬͯΔɽͦͷͨΊɼӈଆͷؔ਺ g ͸೚ҙʹબͿ. 2.1 ඇྵͷ σi ͕Ճࢉແ‫͋Ͱݸݶ‬Δ৔߹ ∗. ࠷ॳʹɼK K ͷ 1 ͭͷ‫ݻ‬༗ϖΞ. (σi2 , vi ). ؔ਺ ui Λఆٛ͢Δɽ ⓒ 2018 Information Processing Society of Japan. ͜ͱ͕Ͱ͖ͳ͍ɽղ͕ଘࡏ͢Δ͜ͱΛอূ͢ΔͨΊɼg ΋ ʹରͯ͠ɼ࣍ͷ. {ui }∞ i=1 ͷுΔۭؒͷதʹͳ͍ͱ͍͚ͳ͍ɽ͜ͷ࣌ɼg ͸࣍ ͷల։Λ࣋ͭɽ. 2.

(3) Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report ∞ . g=. g, ui ui. (17). i=1. ࣜ (16) ͱࣜ (17) Λ߹ΘͤΔͱɼํఔࣜ (1) ͸࣍ࣜͷΑ͏ ʹͳΔɽ ∞ . N ΑΓେ͖͍ i ʹରͯ͠ɼui Λ KK∗ ͷ 0 ʹରԠ͢Δ‫ݻ‬༗ ؔ਺ͱ͢Ε͹ɼ͕࣍ࣜ੒Γཱͭ͜ͱʹͳΔɽ. K∗ Kvi = KK∗ ui = 0, i > N. ΑͬͯɼKvi , Kvi  = K∗ Kvi , vi  = 0 Ͱ͋Δ͜ͱΑΓɼ. σi f, vi ui (x) =. i=1. ∞ . g, ui ui (x). (18). i=1. ࣜ (18) ͷ྆ଆͷ ui ͷ܎਺Λൺֱ͢Δͱɼ࣍ͷ͜ͱ͕Θ ͔Δɽ. Kvi = 0 Ͱ͋Δ͜ͱ͕Θ͔Δɽಉ༷ʹɼK∗ ui = 0 ΋੒Γཱ ͭɽͭ·Γɼi > N ͷ࣌ɼࣜ (14) ͕੒ΓཱͪɼͦΕʹଓ͘ ಉ͡ཧ࿦Ͱɼࣜ (19) ͷલ൒ σi f, vi  = g, ui  ͕ಘΒΕΔɽ ͜ͷ࣌ɼࣜ (20) ͷΑ͏ͳ‫ Ͱ਺ڃ‬f Λද͢͜ͱ͕Ͱ͖ͳ͍ ͕ɼi > N ͷ i ʹରͯ͠ɼf, vi  ͸೚ҙͷ஋ΛऔΔ͜ͱ͕. σi f, vi  = g, ui . Ͱ͖Δɽͭ·Γɼ͜ͷ৔߹͸ɼղ͕ҰҙͰ͸ͳ͍ɽ͔͠͠ɼ. σi−1 g, ui . ⇒ f, vi  =. (19). ࠷‫ʹޙ‬ɼf ͷ vi ʹΑͬͯల։͢Δͱɼσi ɼui ɼvi Λ༻͍ͯ. i > N Ͱ͋Δ i ʹରͯ͠ɼf, vi  = 0 ʹ͢Δͱɼ1 ͭͷղ f ͕ಘΒΕΔɽ࣮͸ɼ͜Ε͕ Kf = g Λຬͨ͢ f ͷதͰϊϧ Ϝ࠷খͷ΋ͷͰ͋Δɽ. ղ f Λදࣔ͢Δ͜ͱ͕Ͱ͖Δɽ. f =. ∞ . f = fN =. f, vi vi. ⇒f =. ∞  i=1. (20). i→∞. σi−1 g, ui vi ͕ൃࢄ͢ΔΑ͏ʹ‫͑ݟ‬ΔͷͰɼશମͷ‫਺ڃ‬΋ൃ 2. ࢄ͢ΔΑ͏ʹ‫͑ݟ‬Δɽ͔͠͠ɼK(x, y) ∈ L ([a, b] × [a, b]) 2. 2. Ͱ͋Ε͹ɼ࡞༻ૉ K : L [a, b] → L [a, b] Λఆٛ͢Δ͜ ͱ͕Ͱ͖ɼ೚ҙͷ g ∈ R(K)(⊂ L2 [a, b]) ʹରͯ͠ɼඞͣ. Kf = g, f ∈ L2 [a, b] ͱͳΔ‫ ૾ݪ‬f ͕ଘࡏ͢Δɽ্‫ه‬ΑΓ f ͸ɼࣜ (20) ͷΑ͏ͳ‫ܗ‬Λ࣋ͭɽf ͕ L2 [a, b] ͷ‫͋Ͱݩ‬Δ͜ ͱΑΓɼL2 ϊϧϜ͕༗‫ͳݶ‬ͷͰɼࣜ (20) ͷӈଆͷ‫͕਺ڃ‬ ඞͣऩଋ͢Δɽ ࣜ (20) ͷӈଆ͕ऩଋ͢Δ࣌ɼ͢ͳΘͪɼk → ∞ ͷ࣌ɼ ‫਺ڃ‬ͷલ k ߲Λআ͍ͨୈ k + 1 ߲͔Βͷ૯࿨͕ 0 ʹऩଋ͢ Δɽͭ·Γɼ͕࣍ࣜ੒Γཱͭɽ. lim. σi−1 g, ui vi = 0. (24). ͱ͕Θ͔Δɽ. 3. Lanczos ๏ + TSVD ๏ ࠷΋ࣗવͳ཭ࢄԽͷߟ͑ํ͸ɼRiemann ࿨Λ࢖ͬͯࣜ. (1) Λ཭ࢄԽ͠ɼઢ‫ํܗ‬ఔࣜ Ax = b ΛಘΔ͜ͱͰ͋Δɽ࿈ ଓͷ৔߹ͱಉ༷ʹߦྻ A ͷಛҟ஋ͱಛҟϕΫτϧΛ༻͍ͯ ղ x ͷۙࣅ஋Λ‫ٻ‬ΊΔɽ. xk =. k  i=1. σi−1 (u∗i b)v i. (25). ͜͜Ͱɼ΄ΜͷҰ෦ͷಛҟ஋ͱಛҟϕΫτϧ͕ඞཁͳͷͰɼ ߦྻ A ʹରͯ͠ Lanczos ๏͕࢖͑Δɽଟ਺ͷಛҟ஋͕ 0 ʹ ͍ۙͷͰɼҰൠʹ Lanczos ๏ͷऩଋ͕଎͍ɽ. ˆ1 ͱ u ˆ 1 = Aˆ Lanczos ๏͸೚ҙͷϕΫτϧ v v 1 /Aˆ v1  ͔ Β࢝·Γɼ࣍ͷ൓෮Λߦ͏͜ͱʹͳΔ [3]ɽ. (21). k+1. ˆ i−1 αi−1 , ˆ i = A∗ u ˆ i−1 − v v ˆi = v ˆ i /βi−1 ˆ v i  = βi−1 , v. ͦͷͨΊɼࣜ (21) ͷӈଆͷલ k ߲ͷ૯࿨͚ͩͰɼ໨ඪͷղ. f ͷۙࣅ஋ fk Λ‫ٻ‬ΊΔ͜ͱ͕Ͱ͖Δɽ f ≈ fk =. σi−1 g, ui vi. ैͬͯɼࣜ (24) Λ͜ͷղͷۙࣅͱͯ͠࢖͏͜ͱ͕Ͱ͖Δ͜. σi−1 g, ui vi. લड़ͷ lim σi = 0 ΑΓɼࣜ (20) ͷӈଆͷ‫਺ڃ‬ͷ߲. ∞ . N  i=1. i=1. k→∞. (23). k  i=1. σi−1 g, ui vi. ˆi = u ˆ i /αi ˆ ui  = αi , u (22). ͜ΕͰɼ୅਺త TSVD ๏ͱಉ༷ʹɼখ͍͞ಛҟ஋Λ੾Γ ࣺͯΔ͜ͱʹΑͬͯɼ࿈ଓͷ৔߹ͷղ f ͷۙࣅ஋Λಛҟ஋ ͱಛҟϕΫτϧͰද͢͜ͱ͕Ͱ͖ͨɽ. 2.2 ඇྵͷ σi ͕༗‫͋Ͱݸݶ‬Δ৔߹ ඇྵͷ σi ͕༗‫͋Ͱݸݶ‬Δ৔߹ɼͦͷ‫਺ݸ‬Λ N ∈ N ͱ ͢Ε͹ɼi > N Ͱ͋Δ͢΂ͯͷ σi = 0 ʹͳΔɽ͜ͷ࣌ɼ. i = 1, 2, · · · , N ʹରͯ͠ɼui ͸લड़ͱಉ༷ʹఆٛͰ͖ɼ KK∗ ͷ σi ʹରԠ͢Δ‫ݻ‬༗ؔ਺Ͱ͋Δ͜ͱʹ͸มΘΒͳ͍ɽ ⓒ 2018 Information Processing Society of Japan. (26). ˆ i−1 βi−1 ˆ i = Aˆ vi − u u. ͨͩ͠ɼ͋Δ βm ͕े෼খ͍͞৔߹ʹऩଋͨ͠ͱ൑ఆ͢Δɽ ͜ͷ࣌ɼ͕࣍ࣜಘΒΕΔɽ . A∗ A. . . Vˆm ˆm U.  =. . Vˆm ˆm U. Hm. . Tm. ͨͩ͠ɼTm ͸֤ αi ͱ βi ͔ΒͳΔ࣍ͷΑ͏ͳ̎ॏର֯ߦ ྻͰɼHm ͸ Tm ͷసஔͰ͋Δɽ ⎞ ⎛ α1 β1 ⎟ ⎜ ⎟ ⎜ .. ⎟ ⎜ . α 2 ∗ ⎟ , H m = Tm Tm = ⎜ ⎟ ⎜ . .. β ⎟ ⎜ m−1 ⎠ ⎝ αm. (27). 3.

(4) Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report. ௨ৗɼm ͸େ͖͘ͳ͍ͷͰɼTm ͷҰൠͷ SVDɿ Tm = ˆm U, Vm = U Σm V ∗ ͕؆୯ʹ‫͖Ͱࢉܭ‬Δɽ࠷‫ ʹޙ‬Um = U ˆ Vm V ͱ͓͚͹ɼߦྻ A ͷ෦෼తͳ SVD ͕ಘΒΕΔɽ. AVm = Um Σm. (28). ͜͜ͰಘΒΕͨಛҟ஋ͱಛҟϕΫτϧΛ༻͍ͯɼࣜ (25) Ͱ ղ x ͷۙࣅ஋Λ‫ٻ‬ΊΔ͜ͱ͕Ͱ͖Δɽ. ˆ i−1 − v ˆ i−1 αi−1 , ˆ i = A∗ W u v ˆi = v ˆ i /βi−1 ˆ v i W = βi−1 , v ˆi = u ˆ i /αi ˆ ui W = αi , u ˆi ͱ v ˆ i ͸ɼຊ౰ʹਖ਼‫ن‬௚ަͳϕ ࣜ (32) Ͱੜ੒͞ΕΔ֤ u Ϋτϧͳͷ͔Λ͜͜Ͱ͔֬ΊΔɽ͋ΔεςοϓͰ͢Ͱʹಘ. ͔͠͠ɼRiemann ࿨͸ੵ෼ͷ཭ࢄԽ๏ͱͯ͠ਫ਼౓͕ͦ Ε΄ͲΑ͍Θ͚Ͱ͸ͳ͍ɽΑΓਫ਼౓ͷ͍͍ੵ෼ެࣜ͸ɼ. Boole ͷެ͕ࣜߟ͑ΒΕΔɽBoole ͷެࣜΑΓ x0 ͱ xn ͷ ؒͷؔ਺ f (x) ͷੵ෼͸ɼ2 ͭͷ୺఺ͱͦͷؒͷ n ౳෼఺. ˆ2, · · · , v ˆi ͱ u ˆ 2, · · · , u ˆ i ͕ਖ਼‫ن‬௚ަͰ͋Δ ˆ1, v ˆ 1, u ΒΕͨ v ˆ i+1 ͕ಘΒΕΔɽ ͱԾఆ͢Δɽͦͯ͠ɼࣜ (32) Ͱ৽͍͠ v ˆ i+1 ͱ v ˆ j ͷ಺ੵΛऔΔͱɼ j = 1, 2, · · · , i − 2 ʹରͯ͠ɼv ࣍ࣜͷΑ͏ʹͳΔɽ. x1 , x2 , · · · , xn−1 ʹ͓͚Δؔ਺஋Λ࢖͑͹࣍ͷΑ͏ͳۙࣅ ͕Ͱ͖Δɽͨͩ͠ɼh = 1/nɽ  b n 2  h f (x)dx ≈ wi f (xi ) 45 i=0 a ⎧ ⎪ 7 (i = 0 or n) ⎪ ⎪ ⎪ ⎨ 14 (i = 4k) wi = ⎪ 32 (i = 4k + 1 or 4k + 3) ⎪ ⎪ ⎪ ⎩ 12 (i = 4k + 2). ˆ j W = v ˆ ∗j W v ˆ i+1 = ˆ v i+1 , v. 1 1 ˆ j )∗ W u ˆ i = (αj u ˆi ˆ ∗j + βj−1 u ˆ ∗j−1 )W u (AW v βi βi =0 (33) ˆ i+1 ͱ v ˆ i ͷ಺ੵΛऔΔͱ࣍ʹͳΔɽ ·ͨɼv (29). ˆi = v ˆ ∗i W v ˆ i+1 = ˆ v i+1 , v. 1 ˆ i )∗ W u ˆ i − αi ) ((AW v βi 1 ˆ i − αi ) ˆ ∗i + βi−1 u ˆ ∗i−1 )W u = ((αi u βi 1 = (αi − αi ) = 0 βi. K(xi , yj )(i, j = 0, 1, · · · , n) ͔ΒͳΔߦྻͱ͢Δɽͦͯ͠ɼ ॏΈΛද͢ߦྻ W Λ࣍ͷΑ͏ʹఆٛ͢Δɽ. (30). ͜͜Ͱɼੵ෼࡞༻ૉ K ͷ཭ࢄԽ͸ AW Ͱද͢͜ͱ͕Ͱ͖ɼ ಘΒΕͨઢ‫ํܕ‬ఔࣜ͸ AW x = b ͱͳΔɽ Ұ‫ݟ‬ɼ͜ͷΞϧΰϦζϜͷߦྻ A ͷͱ͜Ζʹ AW Λ୅ ೖͯ͠‫͚͍ͯ͠ࢉܭ‬͹ྑ͍Α͏ʹ‫͑ݟ‬Δ͕ɼͦΕΛ࣮ࡍʹ ࣮ߦͯ͠ΈΔͱɼ๬·͍݁͠ՌΛಘΔ͜ͱ͕Ͱ͖ͳ͔ͬͨɽ ͦͷཧ༝͸ɼ΋͠ߦྻ AW ΛલͷΞϧΰϦζϜʹ௚઀୅ ೖ͢Δͱɼ࡞༻ૉ K∗ ʹରԠ͢Δߦྻ͕ (AW )∗ = W A∗ ʹ. a. (34). ˆ i+1 ͕લͷ͢΂ ࣜ (33) ͱࣜ (34) ΑΓɼ৽͘͠ಘΒΕͨ v ˆ j (j ≤ i) ͱ௚ަ͢Δɽಉ༷ͳٞ࿦Ͱɼu ˆ i+1 ͸͢΂ͯ ͯͷ v ˆ j (j ≤ i) ͱ௚ަ͢Δ͜ͱ͕Θ͔Δɽैͬͯɼࣜ (33) Ͱ ͷu n. n. ੜ੒͞ΕΔ {ˆ ui }i=1 ͱ {ˆ v i }i=1 ͸ɼͦΕͧΕਖ਼‫ن‬௚ަྻʹ ͳΔɽ લͱಉ͡ɼ͋Δ βi ͕े෼খ͍࣌͞ɼΞϧΰϦζϜ͕ऩ ଋͨ͠ͱ൑ఆ͢Δɽऩଋͨ࣌͠ɼલͱࣅͨΑ͏ͳ͕ࣜಘΒ ΕΔɽ . A∗ W AW. (31). 1 ∗ ˆ i − αi v ˆ W (A∗ W u ˆi) v βi i. =. ·ͣɼx0 = y0 = a, xn = yn = b ͱ͠ɼߦྻ A Λ֤. ͳΔɽ͔͠͠ɼK∗ ͸ɼ࣍ࣜͰ‫ه‬ड़Ͱ͖Δɽ  b ∗ K g= K(x, y)g(x)dx. 1 ∗ ˆ i − αi v ˆ W (A∗ W u ˆi) v βi j. =. ͨͩ͠ɼk ∈ N. ࣜ (29) ʹैͬͯ཭ࢄԽΛߦ͏ͳΒɼ. W = diag{w0 , w1 , · · · , wn }. (32). ˆi − u ˆ i−1 βi−1 ˆ i = AW v u. . . Vˆm ˆm U.  =. . Vˆm ˆm U. Hm. . Tm. ͨͩ͠ɼTm ͱ Hm ͸લड़ͱಉ͡΋ͷͰ͋Δɽ. K∗ ʹରԠ͢Δߦྻ͸ A∗ W ʹͳΔ͸ͣͰ͋ΔɽAW ͕ର. ࣍͸લड़ͱಉ͡ Tm ͷ௨ৗͷಛҟ஋෼ղ Tm = U Σm V ∗ ˆm U, Vm = Vˆm V ͱஔ͘ͱɼ্‫ه‬ͷؔ Λ‫ͯ͠ࢉܭ‬ɼUm = U. শͰ͸ͳ͍‫ݶ‬Γɼ྆ํ͕Ұக͠ͳ͍ɽͦͷͨΊɼ͜͜Ͱໃ. ܎ࣜΛར༻ͯ͠ɼ͕࣍ࣜಘΒΕΔɽ. ‫ʹނ‬ɼ΋ࣜ͠ (31) ͷੵ෼ެࣜͰ཭ࢄԽΛߦ͏ͱɼ࡞༻ૉ. ६͕ੜ͡Δɽ ͜ͷ໰୊Λղܾ͢ΔͨΊʹɼLanczos ๏ͷमਖ਼Λߟ͑Δɽ ·ͣɼੵ෼ެࣜʹରԠͰ͖Δ W Ͱఆ·Δ಺ੵͱϊϧϜΛɼ. = Vˆm V Σm U ∗ U = Vm Σm ˆ m Tm V AW Vm = AW Vˆm V = U. ࣍ͷΑ͏ʹఆٛ͢Δɽ. u, vW = u∗ W v,. ˆm U = Vˆm T ∗ U A∗ W U m = A ∗ W U m. ||u||W =.  u, u,. ∀u, v ∈ Rn. ͜ͷ৽͍͠಺ੵͱϊϧϜͷಋೖʹΑͬͯɼLanczos ๏ͷ൓. ˆ 1 /AW v ˆ 1 W ͔Β࢝ ˆ1 ͱ u ˆ 1 = AW v ෮͸೚ҙͷϕΫτϧ v. ˆ m U Σm V ∗ V = U m Σ m = U ∗ ˆm U = U ∗ U = I ˆ∗ WU Um W Um = U ∗ U m. Vm∗ W Vm = V ∗ Vˆm∗ W Vˆm V = V ∗ V = I. ·Γɼຖճͷ൓෮͸࣍ͷΑ͏ʹͳΔɽ. ैͬͯɼ͜͜ͰಘΒΕͨ Um , Vm , Σm ͸͔֬ʹ W ʹಋ͔. ⓒ 2018 Information Processing Society of Japan. 4.

(5) Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report. . ΕΔ಺ੵͱϊϧϜͷҙຯͰߦྻ A ͷಛҟϕΫτϧͱಛҟ஋. sin(xy)f (y)dy =. ͔ΒͳΔߦྻͰ͋ΔɽಛʹɼલͷΑ͏ʹ‫ʹ͍ޓ‬ໃ६͢Δ͜ ͱ͕ͳ͍ɽ࢒Γ͸ࣜ (25) ʹԊͬͯۙࣅ஋Λ‫ٻ‬ΊΕ͹Α͍ɽ. 1 0. sin x − x cos x x2. ͨͩ͠ɼਅͷղ͸ f (y) = y Ͱ͋Δɽ. W ʹಋ͔ΕΔ಺ੵͱϊϧϜʹΑͬͯɼLanczos ൓෮Λमਖ਼. લͷྫ୊ͱಉ͡ɼ2 ͭͷํ๏Ͱ཭ࢄԽΛߦ͍ɼ‫ݹ‬యతͳ. ͯ͠ɼࣜ (29) ͳͲͷੵ෼ެࣜΛར༻ͯ͠཭ࢄԽͨ͠໰୊Λ. Lanczs ๏ͱमਖ਼൛ͷ࣮ߦ݁ՌΛௐ΂ͨɽͨͩ͠ɼࠓճͷӈ. ͏·͘ղ͚͹Α͍ɽ. ଆͷؔ਺ g(x) ͷ෼฼͕ x2 Ͱ͋ΔͨΊɼb0 = g(0) Λ௚઀. 4. ਺஋࣮‫ݧ‬. ‫͢ࢉܭ‬Δ͜ͱ͕Ͱ͖ͳ͍ͷͰɼ࣍ͷΑ͏ʹ b0 Λ 0 ʹ͓͚ Δ g(x) ͷ‫ͨ͠ࢉܭ͍͓ͯͱݶۃ‬ɽ. ਺஋࣮‫ݧ‬͸࣍ͷΑ͏ͳ‫ͨͬߦͰڥ؀ࢉܭ‬ɽ. b0 = lim. OS: Windows 10 Home(64-bit)ɼ. x→0. CPU: Intel Core i7-6700HQ CPU @ 2.60GHzɼ Memory: 16.0GBɼ. ྫ୊ 2 ͷ࣮ߦ݁ՌΛද 2 ʹ‫ه‬ड़ͨ͠ɽ·ͨɼ2 ͭͷํ๏ Ͱ‫ٻ‬Ίͨ݁Ռʹ‫·ؚ‬ΕΔ‫ࠩޡ‬͸ਤ 3 ʹࣔͨ͠ɽྫ୊ 1 ͱಉ. Program Language: MATLAB R2016aɽ. ༷ʹɼमਖ਼ͨ͠ Lanczos ๏͸ಉ͘͡Β͍ͷ࣌ؒͰ௨ৗͷ 3 ഒҎ্ͷਫ਼౓͕ಘΒΕͨɽ. 4.1 ྫ୊ 1 ࣍ͷੵ෼ํఔࣜΛߟ͑Δɽ  1 ex+1 − 1 exy f (y)dy = x+1 0. 4.3 ྫ୊ 3. ͨͩ͠ɼਅͷղ͸ f (y) = ey Ͱ͋Δɽ ͜͜Ͱ࢖͏ॏΈΛද͢ߦྻ W ͸ࣜ (30) Ͱఆٛ͞Εͨ΋ ͷΛ࢖͏ɽn = 2048, h = 1/n ͱ͢ΔͱɼA ͱ b ͸ҎԼͷ Α͏ʹͳΔɽ. ࣍ͷํఔࣜΛߟ͑Δɽ  1 5x2 − 5x + 3 (x − y)2 f (y)dy = 15 0 ͨͩ͠ɼਅͷղ͸ f (y) = 16y 2 − 16y + 3 Ͱ͋Δɽ. 2 ͭͷ‫ࠩޡࢉܭ‬ͷ݁ՌΛਤ 3 ʹࣔͨ͠ɽ࣍ʹ‫ؒ࣌ࢉܭ‬ͷ ൺֱΛද 3 ʹ‫ه‬ड़ͨ͠ɽࠓճͷ৔߹ɼ‫ͨͬ·ٻ‬ಛҟ஋ͷ‫ݸ‬. xi = yi = ih, i = 0, 1, · · · , n ⎛ e x 0 y0 e x 0 y 1 · · · e x 0 yn ⎜ xy ⎜ e 1 0 e x 1 y 1 · · · e x 1 yn ⎜ A = ⎜ .. .. .. ⎜ . . . ··· ⎝ x n y0 x n y1 x n yn e e ··· e b = (b0 , b1 , · · · , bn )∗ , bi =. sin x − x cos x x sin x sin x = lim =0 = lim x→0 x→0 2 x2 2x. ਺͕গͳͯ͘ɼ‫ݹ‬యతͳ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬͸લͷ. ⎞. ྫ୊ͱͦΕ΄ͲมΘΒͳ͍͕ɼ࢒ࠩͷখ͍͞ղΛಘΔ͜ͱ. ⎟ ⎟ ⎟ ⎟ ⎟ ⎠. exi +1 − 1 , xi + 1. ʹࣦഊͨ͠ɽҰํɼमਖ਼ͨ͠ Lanczos ๏Λར༻͢Δͱɼ࢒ ͕ࠩґવͱͯ͠খ͍͚ͩ͞Ͱͳ͘ɼ΄΅‫׬‬શʹਅͷղͱҰ க͢Δ‫ࢉܭ‬ղ͕ಘΒΕͨɽ. i = 0, 1, · · · , n. ͜ΕҎ߱ͷྫ୊΋ಉ͡Α͏ͳํ๏Ͱ཭ࢄԽΛߦ͏΋ͷͱ. ࢀߟจ‫ݙ‬ [1]. ͢Δɽ લઅͰड़΂ͨ‫ݹ‬యతͳ Lanczos ๏Λద༻ͨ͠ΞϧΰϦζ Ϝͱमਖ਼ͨ͠ Lanczos Λద༻ͨ͠ΞϧΰϦζϜΛͦΕͧ. [2]. Ε࣮ߦͯ͠ɼ࣮ߦ݁Ռ͸ද 1 ʹࣔͨ͠ɽ·ͨɼ֤ yi ʹ͓ ͚Δ‫ ࠩޡ‬e(yi ) = |fexact (yi ) − fnum (yi )| Λਤ 1 ʹϓϩοτ ͨ͠ɽ ද 1 ͱਤ 1 ͔Βɼ‫ݹ‬యతͳ Lanczos ๏ʹ͓͍ͯ΋ɼf (y) =. [3] [4]. y. e ͷ͖Ε͍ͳ‫͕ܗ‬ಘΒΕͨͱ͸͍͑ɼࡉ͔͘‫ࠩޡ‬Λ‫͠ࢉܭ‬ ͯΈΔͱɼਫ਼౓͕ͦΜͳʹ͍͍ͱ͸‫͍͕͍ͨݴ‬ɽͦΕ͸ൺ ֱతʹ‫͕ࠩޡ‬େ͖͍ Riemann ࿨Ͱ཭ࢄԽ͔ͨ͠ΒͰ͋Δɽ ҰํɼBoole ͷެࣜΛར༻ͨ͠मਖ਼൛ͷ Lanczos ͸ɼ‫ݹ‬య తͳ Lanczos ๏ʹൺ΂ͯ 3 ഒҎ্ͷਫ਼౓Λ࣮‫ͨ͠ݱ‬ɽn ͱ. [5] [6]. Silvia Noschese, Lothar Reichel, “A modified truncated singular value decomposition method for discrete illposed problems,” Numer. Linear Algebra Appl. 2014; 21: pp. 813–822. Robert Craig Schmidt, “The numerical solution of linear first kind Fredholm integral eqnarrays using an iterative method,” Iowa State University Digital Repository. 1987; pp. 73–81. Lloyd N. Trefethen, “Numerical Linear Algebra,” SIAM. 2007; pp. 414–415. Hong du, “Approximate solution of the Fredholm integral eqnarray of the first kind in a reproducing kernel Hilbert space,ʡɹ An International Journal of Rapid Publication 2008: 21, pp. 617–623. Martin Hanke,“A Taste of Inverse Problems Basic Theory and Examples,” SIAM. 2017; pp. 12-13,130–132. Paul Garrett: “Compact operators, Hilbert-Schmidt operators,” March 2012. pp. 2–3.. m, k ͷ஋͕ಛʹେ͖͘ͳ͍ͨΊɼ2 ͭͷํ๏ͱ΋࣮ߦ࣌ؒ ͕͔ͳΓ୹ͯ͘ɼແࢹͰ͖Δ΄ͲͰ͋Δɽ. 4.2 ྫ୊ 2 ࣍ͷํఔࣜΛߟ͑Δɽ ⓒ 2018 Information Processing Society of Japan. 5.

(6) Vol.2018-HPC-163 No.4 2018/2/28. ৘ใॲཧֶձ‫ڀݚ‬ใࠂ IPSJ SIG Technical Report. ද 1: ྫ୊ 1 ͷ࣮ߦ݁Ռͷൺֱ m. k. ࢒ࠩ. ɹ૬ର‫ࠩޡ‬. ࣮ߦ࣌ؒ (sec). ‫ݹ‬యతͳ Lanczos ๏ɹ. 10. 7. 2.5300 × 10−15. 2.7100 × 10−3. 0.2331s. मਖ਼ Lanczos ๏. 10. 6. 8.9763 × 10−16. 3.3327 × 10−10. 0.2030s. ද 2: ྫ୊ 2 ͷ࣮ߦ݁Ռͷൺֱ m. k. ࢒ࠩ. ɹ૬ର‫ࠩޡ‬. ࣮ߦ࣌ؒ (sec). ‫ݹ‬యతͳ Lanczos ๏ɹ. 7. 4. 9.5246 × 10−14. 2.5202 × 10−3. 0.1953s. मਖ਼ Lanczos ๏. 7. 4. 1.4434 × 10−14. 2.9982 × 10−10. 0.1667s. ද 3: ྫ୊ 3 ͷ࣮ߦ݁Ռͷൺֱ m. k. ࢒ࠩ. ɹ૬ର‫ࠩޡ‬. ࣮ߦ࣌ؒ (sec). ‫ݹ‬యతͳ Lanczos ๏ɹ. 2. 2. 3.2057 × 10−4. 1.8213 × 10−3. 0.1175s. मਖ਼ Lanczos ๏. 2. 2. 2.3977 × 10−15. 1.2275 × 10−15. 0.0766s. 2.5. 0.035 0.03. ×10-9. 2. 0.025 1.5 0.02 1. e(y). e(y). 0.015 0.01. 0.5. 0.005. 0. 0 -0.5. -0.005 -0.01. 0. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6. 0.7. 0.8. 0.9. -1. 1. 0. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6. 0.7. 0.8. 0.9. 1. y. y. (a) ‫ݹ‬యతͳ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. (b) मਖ਼ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. ਤ 1: ྫ୊ 1 ͷ Lanczos ๏ʹΑΔղͷ‫ࠩޡࢉܭ‬ͷ݁Ռ 9. ×10. -3. ×10. 8. -10. 8 6 7 4. 6. e(y). e(y). 5 2. 4 0. 3 2. -2 1 0. 0. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6. 0.7. 0.8. 0.9. -4. 1. 0. 0.1. 0.2. 0.3. 0.4. y. 0.5. 0.6. 0.7. 0.8. 0.9. 1. y. (a) ‫ݹ‬యతͳ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. (b) मਖ਼ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. ਤ 2: ྫ୊ 2 ͷ Lanczos ๏ʹΑΔղͷ‫ࠩޡࢉܭ‬ͷ݁Ռ 4. ×10-3 8. ×10-15. 6. 3. 4. 2. 2 1. e(y). e(y). 0 0. -2 -4. -1. -6 -2 -8 -3 -4. -10. 0. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6. 0.7. 0.8. 0.9. 1. y. (a) ‫ݹ‬యతͳ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. -12. 0. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6. 0.7. 0.8. 0.9. 1. y. (b) मਖ਼ Lanczos ๏ʹΑΔղͷ‫ࠩޡ‬. ਤ 3: ྫ୊ 3 ͷ Lanczos ๏ʹΑΔղͷ‫ࠩޡࢉܭ‬ͷ݁Ռ. ⓒ 2018 Information Processing Society of Japan. 6.

(7)

参照

関連したドキュメント

In solving equations in which the unknown was represented by a letter, students explicitly explored the concept of equation and used two solving methods.. The analysis of

In this paper, we we have illustrated how the modified recursive schemes 2.15 and 2.27 can be used to solve a class of doubly singular two-point boundary value problems 1.1 with Types

Existence of weak solution for volume preserving mean curvature flow via phase field method. 13:55〜14:40 Norbert

Namely, in [7] the equation (A) has been considered in the framework of regular variation, but only the case c = 0 in (1.4) has been considered, providing some asymptotic formulas

The objective of this paper is to apply the two-variable G /G, 1/G-expansion method to find the exact traveling wave solutions of the following nonlinear 11-dimensional KdV-

In recent years, singular second order ordinary differential equations with dependence on the first order derivative have been studied extensively, see for example [1-8] and

Abstract. Recently, the Riemann problem in the interior domain of a smooth Jordan curve was solved by transforming its boundary condition to a Fredholm integral equation of the

Based on these results, we first prove superconvergence at the collocation points for an in- tegral equation based on a single layer formulation that solves the exterior Neumann