Confinement dual Meissener effect dual Meissener effect
|
|
- あつとし ひろもり
- 7 years ago
- Views:
Transcription
1 BASED ON WORK WITH KENICHI KONISHI (UNIV. OF PISA) [ TO APPEAR IN NPB]
2 Confinement dual Meissener effect dual Meissener effect
3 1) Perturbed SU(N) Seiberg WiRen theory : 2) SU(N) with Flavors at Higgs Branch root: 3) Pouliot Type duality [ SEIBERG WITTEN `94, DOUGLAS SHENKER `96] [ CARLINO KONISHI KUMAR MURAYAMA `01] [ STRASSLER `98] Q: QCD A: confinement SUSY SUSY
4 SU(N) confinement abelian monopole non abelian monopole Higgsing [ Abelianizacon `80]
5 1) N=1 Pure Yang Mills Theories Review of SUSY vacua GNO duality Wilson `thoof loop `thoof classificacon WiRen effect 2) N=1 SYM with a Higgs field set up electric/magnecc screening Confinement index 3) Conclusion
6 4D N=1 pure Yang Mills dual coxeter number theta angle 2 pi
7 confinement Wilson `thoof Loop?
8 [ GODDARD NUYTS OLIVE `77] Nonabelian monopole electric/magnecc duality GNO claim 1 :
9
10 weight vector weight lajce adjoint weight vector root vector
11 GNO claim 2 : Quanczacon condicon weight vector H root vector H v weight vector Pure Yang Mills adjoint H weight vector
12 electric magnecc adjoint rep. fundamental rep. symmetric tensor rep. anc symmetric tensor rep. non abelian monopole GNO dual
13 Wilson `thoof loop fundamental rep. pure YM Pure SYM gaugino, gluon
14 adjoint R center SU(N) (N ality) N ality
15 Wilson loop N ality N ality
16 Weight vector up to Root vector GNO nonabelian monopole H weight vector magnecc group v
17 Pure YM Wilson thoof Loop
18 Massive vacua [ THOOFT `78 : DONAGI WITTEN `95] skew form mutually local mutually non local
19 1 : (a,b) mutually non local confine 2 : 2 x,y mutually local 3 : massive subgroup
20 N : confining oblique confining Higgs N : N+1 N=6 Mixed
21 electric/magcc charge weight vector theta angle magnecc charge WiRen effect electric charge generate [ KAPUSTIN `05] Simply laced non simply laced Simply laced electric
22 Non Simply laced
23 N N
24
25 Higgs massive Integrate out product pure SYM confine dual coxeter number
26 Wilson Loop k singlet Area law Higgsing electric screening
27 Wilson Loop GNO weight vector
28 Area law
29 electric screening SU(Ni) N1, N2 singlet Area law electric/magnecc screening Area law Wilson Loop Greatest Common divisor t Confinement Index
30 Area Area Area Area theta angle index Dynkin index of embedding
31 thoof Loop dual group thoof Loop dual group
32 external charge singlet magnecc screening Area law confinement index 2
33 singlet electric screening Area [ AUZZI BOLOGNESI EVSLIN KONISHI MURAYAMA `04] Area law
34 SU(N) N singlet confinement index Area law Nontrivial r theta angle U(N) USp Dynkin index of embedding U(N) theta angle confinement index
35 N=1 Wilson `thoof Loop confinement index t order t subgroup confinement index t G theta angle SW Wilson `t Hoof loop? Wilson t Hoof loop
36 [ ASHOK CACHAZO DELL AQUILLA `06] Work in Progress with PI friends
37 Higgs SUSY vacua SUSY breaking vacua SUSY breaking vacua SUSY SUSY breaking vacua index descripcon SW, Konishi Anomaly, Seiberg dual consistency check
38 Perimeter law Area law Perimeter law Area law Perimeter law Area law
39 confinement confinement Wilson thoof Loop QCD subgroup confinement Landscape of field theories superpotencal
40 Wilson thoof Loop confinement index SU(N) with adjoint [ CACHAZO SEIBERG WITTEN`03 ] confinement index open problem ( talk)
41 confinement index 1
Seiberg Witten 1994 N = 2 SU(2) Yang-Mills 1 1 3 2 5 2.1..................... 5 2.2.............. 8 2.3................................. 9 3 N = 2 Yang-Mills 11 3.1............................... 11 3.2
More informationSUSY DWs
@ 2013 1 25 Supersymmetric Domain Walls Eric A. Bergshoeff, Axel Kleinschmidt, and Fabio Riccioni Phys. Rev. D86 (2012) 085043 (arxiv:1206.5697) ( ) Contents 1 2 SUSY Domain Walls Wess-Zumino Embedding
More informationYITP50.dvi
1 70 80 90 50 2 3 3 84 first revolution 4 94 second revolution 5 6 2 1: 1 3 consistent 1-loop Feynman 1-loop Feynman loop loop loop Feynman 2 3 2: 1-loop Feynman loop 3 cycle 4 = 3: 4: 4 cycle loop Feynman
More informationq quark L left-handed lepton. λ Gell-Mann SU(3), a = 8 σ Pauli, i =, 2, 3 U() T a T i 2 Ỹ = 60 traceless tr Ỹ 2 = 2 notation. 2 off-diagonal matrices
Grand Unification M.Dine, Supersymmetry And String Theory: Beyond the Standard Model 6 2009 2 24 by Standard Model Coupling constant θ-parameter 8 Charge quantization. hypercharge charge Gauge group. simple
More informationYang-Mills Yang-Mills Yang-Mills 50 operator formalism operator formalism 1 I The Dawning of Gauge T
Yang-Mills 50 E-mail: kugo@yukawa.kyoto-u.ac.jp 2004 Yang-Mills 50 2004 Yang-Mills 50 operator formalism operator formalism 1 I The Dawning of Gauge Theory O Raifeartaigh [1] I, II, III O Raifeartaigh
More information(Tokyo Institute of Technology) Seminar at Ehime University ( ) 9 3 U(N C ), N F /2 BPS ( ) 12 5 (
(Tokyo Institute of Technology) Seminar at Ehime University 2007.08.091 1 2 1.1..................... 2 2 ( ) 9 3 U(N C ), N F 11 4 1/2 BPS ( ) 12 5 ( ) 19 6 Conclusion 23 1 1.1 GeV SU(3) SU(2) U(1): W
More informationN=1 N=1 QCD N=1 non-abelian QCD X 0
2 945207 18 9 22 N=1 N=1 QCD N=1 non-abelian QCD X 0 1 3 2 7 2.1..................................... 7 2.2.................................. 8 2.3............ 10 2.4 moduli...............................
More information( ) : (Technocolor)...
( ) 2007.5.14 1 3 1.1............................. 3 1.2 :........... 5 1.3........................ 7 1.4................. 8 2 11 2.1 (Technocolor)................ 11 2.2............................. 12
More informationLarge N Reduction for Gauge Theories on 3-sphere
伊敷吾郎 ( 大阪大学 & KEK) 以下の論文に基づく arxiv:0807.2352[hep-th], Phys. Rev. D78:106001,2008. T.Ishii (Osaka U.), GI, S. Shimasaki (Osaka U.) and A. Tsuchiya (Shizuoka U.) arxiv:0810.2884[hep-th], to appear in PRL.
More informationIntroduction SFT Tachyon condensation in SFT SFT ( ) at 1 / 38
( ) 2011 5 14 at 1 / 38 Introduction? = String Field Theory = SFT 2 / 38 String Field : ϕ(x, t) x ϕ x / ( ) X ( σ) (string field): Φ[X(σ), t] X(σ) Φ (Φ X(σ) ) X(σ) & / 3 / 38 SFT with Lorentz & Gauge Invariance
More information' , 24 :,,,,, ( ) Cech Index theorem 22 5 Stability 44 6 compact 49 7 Donaldson 58 8 Symplectic structure 63 9 Wall crossing 66 1
1998 1998 7 20 26, 44. 400,,., (KEK), ( ) ( )..,.,,,. 1998 1 '98 7 23, 24 :,,,,, ( ) 1 3 2 Cech 6 3 13 4 Index theorem 22 5 Stability 44 6 compact 49 7 Donaldson 58 8 Symplectic structure 63 9 Wall crossing
More informationD-brane K 1, 2 ( ) 1 K D-brane K K D-brane Witten [1] D-brane K K K K D-brane D-brane K RR BPS D-brane
D-brane K 1, 2 E-mail: sugimoto@yukawa.kyoto-u.ac.jp (2004 12 16 ) 1 K D-brane K K D-brane Witten [1] D-brane K K K K D-brane D-brane K RR BPS D-brane D-brane RR D-brane K D-brane K D-brane K K [2, 3]
More informationNorisuke Sakai (Tokyo Institute of Technology) In collaboration with M. Eto, T. Fujimori, Y. Isozumi, T. Nagashima, M. Nitta, K. Ohashi, K. Ohta, Y. T
Norisuke Sakai (Tokyo Institute of Technology) In collaboration with M. Eto, T. Fujimori, Y. Isozumi, T. Nagashima, M. Nitta, K. Ohashi, K. Ohta, Y. Tachikawa, D. Tong, M. Yamazaki, and Y. Yang 2008.3.21-26,
More information001 No.3/12 1 1 2 3 4 5 6 4 8 13 27 33 39 001 No.3/12 4 001 No.3/12 5 001 No.3/12 6 001 No.3/12 7 001 8 No.3/12 001 No.3/12 9 001 10 No.3/12 001 No.3/12 11 Index 1 2 3 14 18 21 001 No.3/12 14 001 No.3/12
More informationN = , 4 Introduction 3 1 ADHM Construction Notation Yang-Mills Theory
N = 2 2004 8 3, 4 Introduction 3 1 ADHM Construction 5 1.1 Notation..................................... 5 1.2 Yang-Mills Theory............................... 8 1.3 BPST Instanton................................
More informationPowerPoint プレゼンテーション
0 1 2 3 4 5 6 1964 1978 7 0.0015+0.013 8 1 π 2 2 2 1 2 2 ( r 1 + r3 ) + π ( r2 + r3 ) 2 = +1,2100 9 10 11 1.9m 3 0.64m 3 12 13 14 15 16 17 () 0.095% 0.019% 1.29% (0.348%) 0.024% 0.0048% 0.32% (0.0864%)
More information3 exotica
( / ) 2013 2 23 embedding tensors (non)geometric fluxes exotic branes + D U-duality G 0 R-symmetry H dim(g 0 /H) T-duality 11 1 1 0 1 IIA R + 1 1 1 IIB SL(2, R) SO(2) 2 1 9 GL(2, R) SO(2) 3 SO(1, 1) 8
More informationuntitled
20 7 1 22 7 1 1 2 3 7 8 9 10 11 13 14 15 17 18 19 21 22 - 1 - - 2 - - 3 - - 4 - 50 200 50 200-5 - 50 200 50 200 50 200 - 6 - - 7 - () - 8 - (XY) - 9 - 112-10 - - 11 - - 12 - - 13 - - 14 - - 15 - - 16 -
More informationuntitled
19 1 19 19 3 8 1 19 1 61 2 479 1965 64 1237 148 1272 58 183 X 1 X 2 12 2 15 A B 5 18 B 29 X 1 12 10 31 A 1 58 Y B 14 1 25 3 31 1 5 5 15 Y B 1 232 Y B 1 4235 14 11 8 5350 2409 X 1 15 10 10 B Y Y 2 X 1 X
More informationスライド 1
The Dual Superconductor Picture of Color Confinement in Gluodynamics 石黒克也 ( 高知大学総合情報センター & 理研 ) 共同研究者 鈴木恒雄 関戸暢 長谷川将康 駒佳明 ( 金沢大学 & 理研 ) ( 沼津高専 ) 2008 年 12 月 26 日九大若手研究会 量子色力学の相構造研究の現状と展望 Color confinement
More information2000 Vol.2 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 Integrate Non- Integrate Operation Creation 42 80 60 40 20 0 74.6 49.2 67.7
More information四変数基本対称式の解放
Solving the simultaneous equation of the symmetric tetravariate polynomials and The roots of a quartic equation Oomori, Yasuhiro in Himeji City, Japan Dec.1, 2011 Abstract 1. S 4 2. 1. {α, β, γ, δ} (1)
More informationkougiroku7_26.dvi
2005 : D-brane tachyon : ( ) 2005 8 7 8 :,,,,,,, 1 2 1.1 Introduction............................... 2 1.2......................... 6 1.3 Second Revolution (1994 )................... 11 2 Type II 26 2.1
More informationnakayama.key
2017/11/1@Flavor Physics Workshop 2017 Contents CP 1932 10 4 p + p! p + p + p + p P. Blasi, 1311.7346 d d. 10 Gpc 10 0 Cohen, De Rujula, Glashow (1997) d B0 Flux [photons cm -2 s -1 MeV -1 sr -1
More information..0.._0807...e.qxp
4 6 0 4 6 0 4 6 8 30 34 36 38 40 4 44 46 8 8 3 3 5 4 6 7 3 4 6 7 5 9 8 3 4 0 3 3 4 3 5 3 4 4 3 4 7 6 3 9 8 Check 3 4 6 5 3 4 0 3 5 3 3 4 4 7 3 3 4 6 9 3 3 4 8 3 3 3 4 30 33 3 Check Check Check Check 35
More informationh01
P03 P05 P10 P13 P18 P21 1 2 Q A Q A Q A Q A Q A 3 1 check 2 1 2-1 2-2 2-3 2-4 2-5 2-5-1 2-6 2-6-1 2-6-2 2-6-3 3 3-1 3-2 3-3 3-4 3 check 4 5 3-5 3-6 3-7 3-8 3-9 4-1 4-1-1 4-2 4-3 4-4 4-5 4-6 5-1 5-2 4
More information1 2 3 4 1 2 1 2 3 4 5 6 7 8 9 10 11 27 29 32 33 1 2 3 7 9 11 13 15 17 19 21 23 26 CHECK! 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
More information01
2 017 INDEX 01 02 03-04 05 06 07 08 09-10 11-13 14 15 16 17-21 21 22 24 26 27 28 29 30 31 32 34 36 37 38 OSAKA CHILD CARE & HEALTH COLLEGE 01 02 03 04 05 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21
More information.T.C.Y._.E..
25 No.33 C O N T E N T S REVIEW 1 2 5 4 3 6 7 8 9 1 11 1, 1, 7,5 75 916,95 (121) 756,67 (15) 718,89 (13) 91,496 (169) 54,2 (179) 3,243 (75) 727,333 (129) 564,47 (112) 55,458 (11) 6,68,953 (18) 5,624,957
More information0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo t
e-mail: koyama@math.keio.ac.jp 0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo type: diffeo universal Teichmuller modular I. I-. Weyl
More informationネットショップ・オーナー2 ユーザーマニュアル
1 1-1 1-2 1-3 1-4 1 1-5 2 2-1 A C 2-2 A 2 C D E F G H I 2-3 2-4 2 C D E E A 3 3-1 A 3 A A 3 3 3 3-2 3-3 3-4 3 C 4 4-1 A A 4 B B C D C D E F G 4 H I J K L 4-2 4 C D E B D C A C B D 4 E F B E C 4-3 4
More information/9/ ) 1) 1 2 2) 4) ) ) 2x + y 42x + y + 1) 4) : 6 = x 5) : x 2) x ) x 2 8x + 10 = 0
1. 2018/9/ ) 1) 8 9) 2) 6 14) + 14 ) 1 4 8a 8b) 2 a + b) 4) 2 : 7 = x 8) : x ) x ) + 1 2 ) + 2 6) x + 1)x + ) 15 2. 2018/9/ ) 1) 1 2 2) 4) 2 + 6 5) ) 2x + y 42x + y + 1) 4) : 6 = x 5) : x 2) x 2 15 12
More informationEPSON エプソンプリンタ共通 取扱説明書 ネットワーク編
K L N K N N N N N N N N N N N N L A B C N N N A AB B C L D N N N N N L N N N A L B N N A B C N L N N N N L N A B C D N N A L N A L B C D N L N A L N B C N N D E F N K G H N A B C A L N N N N D D
More informationありがとうございました
- 1 - - 2 - - 3 - - 4 - - 5 - 1 2 AB C A B C - 6 - - 7 - - 8 - 10 1 3 1 10 400 8 9-9 - 2600 1 119 26.44 63 50 15 325.37 131.99 457.36-10 - 5 977 1688 1805 200 7 80-11 - - 12 - - 13 - - 14 - 2-1 - 15 -
More informationEPSON エプソンプリンタ共通 取扱説明書 ネットワーク編
K L N K N N N N N N N N N N N N L A B C N N N A AB B C L D N N N N N L N N N A L B N N A B C N L N N N N L N A B C D N N A L N A L B C D N L N A L N B C N N D E F N K G H N A B C A L N N N N D D
More information公務員人件費のシミュレーション分析
47 50 (a) (b) (c) (7) 11 10 2018 20 2028 16 17 18 19 20 21 22 20 90.1 9.9 20 87.2 12.8 2018 10 17 6.916.0 7.87.4 40.511.6 23 0.0% 2008 2009 2010 2011 2012 2013 2014 2015 2016 2017 2018 2.0% 4.0% 6.0% 8.0%
More informationQ1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 A B (A/B) 1 1,185 17,801 6.66% 2 943 26,598 3.55% 3 3,779 112,231 3.37% 4 8,174 246,350 3.32% 5 671 22,775 2.95% 6 2,606 89,705 2.91% 7 738 25,700 2.87% 8 1,134
More information橡hashik-f.PDF
1 1 1 11 12 13 2 2 21 22 3 3 3 4 4 8 22 10 23 10 11 11 24 12 12 13 25 14 15 16 18 19 20 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 144 142 140 140 29.7 70.0 0.7 22.1 16.4 13.6 9.3 5.0 2.9 0.0
More information198
197 198 199 200 201 202 A B C D E F G H I J K L 203 204 205 A B 206 A B C D E F 207 208 209 210 211 212 213 214 215 A B 216 217 218 219 220 221 222 223 224 225 226 227 228 229 A B C D 230 231 232 233 A
More information1
1 2 3 4 5 (2,433 ) 4,026 2710 243.3 2728 402.6 6 402.6 402.6 243.3 7 8 20.5 11.5 1.51 0.50.5 1.5 9 10 11 12 13 100 99 4 97 14 A AB A 12 14.615/100 1.096/1000 B B 1.096/1000 300 A1.5 B1.25 24 4,182,500
More information05[ ]戸田(責)村.indd
147 2 62 4 3.2.1.16 3.2.1.17 148 63 1 3.2.1.F 3.2.1.H 3.1.1.77 1.5.13 1 3.1.1.05 2 3 4 3.2.1.20 3.2.1.22 3.2.1.24 3.2.1.D 3.2.1.E 3.2.1.18 3.2.1.19 2 149 3.2.1.23 3.2.1.G 3.1.1.77 3.2.1.16 570 565 1 2
More informationM5-brane M-theory の 基 本 的 自 由 度 のひとつ (5+1) 次 元 物 体 複 数 枚 かさなると 6 次 元 の 謎 の 超 共 形 場 の 理 論 (2,0)-theory を 生 じる 複 数 のM5-brane の 系 をコンパクト 化 すると... * 低 次 元
4 次 元 ゲージ 理 論 に 隠 れた 2 次 元 共 形 対 称 性 細 道 和 夫 日 本 物 理 学 会 2011 年 秋 季 大 会 2011/09/17 @ 弘 前 大 学 M5-brane M-theory の 基 本 的 自 由 度 のひとつ (5+1) 次 元 物 体 複 数 枚 かさなると 6 次 元 の 謎 の 超 共 形 場 の 理 論 (2,0)-theory を 生 じる
More information!!! 10 1 110 88 7 9 91 79 81 82 87 6 5 90 83 75 77 12 80 8 11 89 84 76 78 85 86 4 2 32 64 10 44 13 17 94 34 33 107 96 14 105 16 97 99 100 106 103 98 63 at 29, 66 at 58 12 16 17 25 56
More informationDaisukeSatow.key
Nambu-Goldstone Fermion in Quark-Gluon Plasma and Bose-Fermi Cold Atom System ( /BNL! ECT* ") : Jean-Paul Blaizot (Saclay CEA #) ( ) (SUSY) = b f b f 2 (SUSY) Q: supercharge b f b f SUSY: [Q, H]=0 Supercharge
More information0. Intro ( K CohFT etc CohFT 5.IKKT 6.
E-mail: sako@math.keio.ac.jp 0. Intro ( K 1. 2. CohFT etc 3. 4. CohFT 5.IKKT 6. 1 µ, ν : d (x 0,x 1,,x d 1 ) t = x 0 ( t τ ) x i i, j, :, α, β, SO(D) ( x µ g µν x µ µ g µν x ν (1) g µν g µν vector x µ,y
More information·«¤ê¤³¤ß·²¤È¥ß¥ì¥Ë¥¢¥àÌäÂê
.. 1 10-11 Nov., 2016 1 email:keiichi.r.ito@gmail.com, ito@kurims.kyoto-u.ac.jp ( ) 10-11 Nov., 2016 1 / 45 Clay Institute.1 Construction of 4D YM Field Theory (Jaffe, Witten) Jaffe, Balaban (1980).2 Solution
More informationIndex P02 P03 P05 P07 P09 P11 P12 P22 01 02
www.rakuten-bank.co.jp/home-loan Index P02 P03 P05 P07 P09 P11 P12 P22 01 02 1 2 3 1 2 3 03 04 1 2 3 4 1.365% 1.05% 1 2 2 3 3 0 1 2 5 7 1 3 5 7 10 20 05 06 POINT 1 POINT 2 POINT 3 POINT 1 POINT 2 07 08
More informationKaluza-Klein(KK) SO(11) KK 1 2 1
Maskawa Institute, Kyoto Sangyo University Naoki Yamatsu 2016 4 12 ( ) @ Kaluza-Klein(KK) SO(11) KK 1 2 1 1. 2. 3. 4. 2 1. 標準理論 物質場 ( フェルミオン ) スカラー ゲージ場 クォーク ヒッグス u d s b ν c レプトン ν t ν e μ τ e μ τ e h
More informationI 1 V ( x) = V (x), V ( x) = V ( x ) SO(3) x = R x: R SO(3) Lorentz R t JR = J: J = diag(1, 1, 1, 1) x = x + a Poincarré ( ) 2
III 1 2005 Jan 30th, 2006 I : II : I : [ I ] 12 13 9 (Landau and Lifshitz, Quantum Mechanics chapter 12, 13, 9: Pergamon Pr.) [ ] ( ) (H. Georgi, Lie algebra in particle physics, Perseus Books) [ ] II
More informationQCD 1 QCD GeV 2014 QCD 2015 QCD SU(3) QCD A µ g µν QCD 1
QCD 1 QCD GeV 2014 QCD 2015 QCD SU(3) QCD A µ g µν QCD 1 (vierbein) QCD QCD 1 1: QCD QCD Γ ρ µν A µ R σ µνρ F µν g µν A µ Lagrangian gr TrFµν F µν No. Yes. Yes. No. No! Yes! [1] Nash & Sen [2] Riemann
More informationあ
Supersymmetry non-renormalization theorem from a computer and the AdS/CFT correspondence 総研大 D1 本多正純 伊敷吾郎氏 ( CQUeST ), Sang-Woo Kim 氏 ( KEK ), 西村淳氏 ( KEK& 総研大 ), 土屋麻人氏 ( 静岡大 ) との共同研究に基づく 2010/7/23 基研研究会
More information格子QCD実践入門
-- nakamura at riise.hiroshima-u.ac.jp or nakamura at an-pan.org 2013.6.26-27 1. vs. 2. (1) 3. QCD QCD QCD 4. (2) 5. QCD 2 QCD 1981 QCD Parisi, Stamatescu, Hasenfratz, etc 2 3 (Cut-Off) = +Cut-Off a p
More information情報処理学会研究報告 IPSJ SIG Technical Report Vol.2013-CVIM-186 No /3/15 EMD 1,a) SIFT. SIFT Bag-of-keypoints. SIFT SIFT.. Earth Mover s Distance
EMD 1,a) 1 1 1 SIFT. SIFT Bag-of-keypoints. SIFT SIFT.. Earth Mover s Distance (EMD), Bag-of-keypoints,. Bag-of-keypoints, SIFT, EMD, A method of similar image retrieval system using EMD and SIFT Hoshiga
More information[ ] = L [δ (D ) (x )] = L D [g ] = L D [E ] = L Table : ħh = m = D D, V (x ) = g δ (D ) (x ) E g D E (Table )D = Schrödinger (.3)D = (regularization)
. D............................................... : E = κ ............................................ 3.................................................
More informationnon-gaussianities de Sitter space non-gaussianities N. Arkani-Hamed, J. Maldacena [arxiv: v1[hep-th]] T. Noumi, M. Yamaguchi, D. Yokoyama [ar
64 2018 8 6 8 11 @ 1 2018 8 7 ( ) 1.1 1 (19:00-22:15) 1.1.1 ( ) 1.1.2 ( ) MSSM MSSM 1.1.3 ( ) ON ANOMALOUS ELECTROWEAK BARYON-NUMBER NON-CONSERVATION IN THE EARLY UNIVERSE (review) ( ) 100 GeV GUT 1.1.4
More information...6...6...7...10...11...12...12...12...12...12...13...13...13...13...13...13...13 NPB...14...14...14...17...19...20...20 MLB NPB...23...25...25...27.
1 ...6...6...7...10...11...12...12...12...12...12...13...13...13...13...13...13...13 NPB...14...14...14...17...19...20...20 MLB NPB...23...25...25...27...29...30...31...32...33 2 34...37...37...37...38...40...40...44...44...45...45...45...45...46...46...46...47...47...48
More informationR R P N (C) 7 C Riemann R K ( ) C R C K 8 (R ) R C K 9 Riemann /C /C Riemann 10 C k 11 k C/k 12 Riemann k Riemann C/k k(c)/k R k F q Riemann 15
(Gen KUROKI) 1 1 : Riemann Spec Z 2? 3 : 4 2 Riemann Riemann Riemann 1 C 5 Riemann Riemann R compact R K C ( C(x) ) K C(R) Riemann R 6 (E-mail address: kuroki@math.tohoku.ac.jp) 1 1 ( 5 ) 2 ( Q ) Spec
More information1 1.1 R (ring) R1 R4 R1 R (commutative [abelian] group) R2 a, b, c R (ab)c = a(bc) (associative law) R3 a, b, c R a(b + c) = ab + ac, (a + b)c = ac +
ALGEBRA II Hiroshi SUZUKI Department of Mathematics International Christian University 2004 1 1 1 2 2 1 3 3 1 4 4 1 5 5 1 6 6 1 7 7 1 7.1....................... 7 1 7.2........................... 7 4 8
More informationOTO研究会スライド
OTO @, 2017 5 26 2 CFT OTO ) PTEP 2016 (2016) no.11, 113B06 (arxiv1602.06542[hep-th]) Collaboration with P. Caputa(YITP) and A.Veliz-Osorio(Queen Mary U.) i i +1 H = X i i z z i+1 + h X i i x i z = 1
More information? FPGA FPGA FPGA : : : ? ( ) (FFT) ( ) (Localization) ? : 0. 1 2 3 0. 4 5 6 7 3 8 6 1 5 4 9 2 0. 0 5 6 0 8 8 ( ) ? : LU Ax = b LU : Ax = 211 410 221 x 1 x 2 x 3 = 1 0 0 21 1 2 1 0 0 1 2 x = LUx = b 1 31
More informationmain.dvi
SGC - 70 2, 3 23 ɛ-δ 2.12.8 3 2.92.13 4 2 3 1 2.1 2.102.12 [8][14] [1],[2] [4][7] 2 [4] 1 2009 8 1 1 1.1... 1 1.2... 4 1.3 1... 8 1.4 2... 9 1.5... 12 1.6 1... 16 1.7... 18 1.8... 21 1.9... 23 2 27 2.1
More informationIsogai, T., Building a dynamic correlation network for fat-tailed financial asset returns, Applied Network Science (7):-24, 206,
H28. (TMU) 206 8 29 / 34 2 3 4 5 6 Isogai, T., Building a dynamic correlation network for fat-tailed financial asset returns, Applied Network Science (7):-24, 206, http://link.springer.com/article/0.007/s409-06-0008-x
More informationuntitled
18 18 8 17 18 8 19 3. II 3-8 18 9:00~10:30? 3 30 3 a b a x n nx n-1 x n n+1 x / n+1 log log = logos + arithmos n+1 x / n+1 incompleteness theorem log b = = rosário Euclid Maya-glyph quipe 9 number digits
More informationCore Ethics Vol. Nerriere D.Hon EU GS NPO GS GS Oklahoma State University Kyoto Branch OSU-K OSU-K OSU-K
Core Ethics Vol. K EU Core Ethics Vol. Nerriere D.Hon EU GS NPO GS GS Oklahoma State University Kyoto Branch OSU-K OSU-K OSU-K OSU-K OSU-K OSU-K OSU-K OSU-K Team FA SA TP TP KINDER WP THP FP, KINDER World
More informationLarge N Reduction for Gauge Theories on 3-sphere
JHEP0611(2006)089 PRD78(2008)106001 PRL102(2009)111601 JHEP0909(2009) 029 JHEP1111 (2011) 036 JHEP1302 (2013) 148 arxiv:1308.3525 Pos LATTICE2010, 253 Pos LATTICE2011, 244 伊敷吾郎 ( 京大基研 ) 以下の論文に基づく Ishiki-Shimasaki-Takayama-Tsuchiya
More information2 2 Belavin Polyakov Zamolodchikov (BPZ) 1984 [13] 2 BPZ BPZ Virasoro [16][18] [20], [30], [47] [1][6] [8][10], [11], [12] Affine [6],GKO [2] W
SGC -83 2 2 Belavin Polyakov Zamolodchikov (BPZ) 1984 [13] 2 BPZ BPZ 1 3 4 Virasoro [16][18] [20], [30], [47] [1][6] [8][10], [11], [12] Affine [6],GKO [2] W [14] c = 1 CFT [8] Rational CFT [15], [56]
More information