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t o c onsider a far br oader c lass of low coor dinate degr ee (L CD ) alg orithms . In fact w e w ill c onsider a slightly br oader c lass of ðð- v alued L CD alg orithms , supplement ed b y an additional r ounding sc heme int o Σð . The r andomized r ounding Ì ð of ð is de- fined b y Ì ð â ðððððœ â ð( ð )... | https://arxiv.org/abs/2505.20607v1 |
is essentially best -possible under the lo w degr ee heuristic. In particular , this heuristic sugg est s fr om the ener gy - degr ee tr adeoff of ð· â€ Ì ð ( ðž ) that finding solutions w ith ener gy ðž r equir es time ðÌ Î© ( ðž ). This tr adeoff is att ainable along the full r ang e 1 ⪠ðž †ð v ia the f ollo w ing... | https://arxiv.org/abs/2505.20607v1 |
em 1. 4 is not able and highly sugg estiv e . See also [L S24] f or r elat ed discussion. W e also mention that c onjectur ally optimal tr ade - off s of a similar fla v or bet w een running time and signal-t o -noise r atio ha v e been est ablished f or spar se PC A in [ A WZ23] , [Din+24] and f or t ensor PC A in [K ... | https://arxiv.org/abs/2505.20607v1 |
f or the E uc lidean ball of r adius ð ar ound ð¥ . In addition, w e w rit e ðµÎ£ ( ð¥ , ð ) â ðµ ( ð¥ , ð ) ⩠Σð = { ðŠ â Σð : â ðŠ â ð¥ â < ð } , t o denot e point s on Σð w ithin dist anc e ð of ð¥ . W e use ð© ( ð , ð2) t o denot e the scalar N ormal distribution w ith giv en mean and v arianc e , and the ... | https://arxiv.org/abs/2505.20607v1 |
( ð ) depends only on ðð } , ð†ð· â span ( { ððœ : ðœ â [ ð ] , | ðœ | †ð· } ) These subset s describe functions whic h only depend on some subset of c oor dinat es , or on some bounded number of c oor dinat es . N ot e that ð[ ð ] = ð†ð = ð¿2( ðð, ðâ ð) . The coor dinate degr ee of a function ð â ð¿2... | https://arxiv.org/abs/2505.20607v1 |
, w e kno w that f or eac h ðð â ð†ð· w e ha v e ( 1 â ð )ð·ð | ðð ( ð ) |2†ð [ ðð ( ð ) ðð ( ðâ²) ] †ð | ðð ( ð ) |2. Summing this o v er ð giv es ( 1 â ð )ð·â€ ð âš ð ( ð ) , ð ( ðâ²) ⩠†1 . C ombining this w ith the abo v e , and using 1 â ( 1 â ð )ð·â€ ð ð· , y ields ( 1. 4) . â¡ R emar k ... | https://arxiv.org/abs/2505.20607v1 |
uppose ð : ððâ ðð is a deterministic alg orithm with pol ynomial degr ee (r esp . coor di- nate degr ee ) ð· and norm ð â ð ( ð ) â2†ð¶ ð . Then, f or ð = ð ( 1 ) and standar d N ormal r . v .s ð and ðâ² whic h ar e ( 1 â ð ) - corr elated (r esp . ( 1 â ð ) -r esampled), Ì ðð as in Definition 1. 8 sat... | https://arxiv.org/abs/2505.20607v1 |
same ar gument pr o v es har dness when ð is a lo w degr ee poly nomial alg orithm; this is omitt ed f or br e v it y .) 2 Har dness f or Lo w Degr ee Alg orithms In this section, w e pr o v e Theor em 1.3 and Theor em 1. 4 â that is , w e e xhibit str ong lo w degr ee har dness f or both lo w poly nomial degr ee and ... | https://arxiv.org/abs/2505.20607v1 |
, sugg esting that a sharp analy sis v ia global OGP ar gument s ma y be c hallenging t o implement. Let us giv e a mor e det ailed outline of our str at egy , in the case of lo w c oor dinat e degr ee . Let ðž be an ener gy le v el, and assume ð is a Σð - v alued alg orithm w ith c oor dinat e degr ee at most ð· †Ì... | https://arxiv.org/abs/2505.20607v1 |
degr ee alg orithms w ithout the r andomized r ounding st ep . T o handle the latt er , w e obser v e that solutions t o a giv en NPP inst anc e ar e isolat ed w ith high pr obabilit y . This implies that r andomized r ounding either c hang es only ð ( 1 ) c oor dinat es ( whic h pr eser v es st abilit y ), or else in... | https://arxiv.org/abs/2505.20607v1 |
1 â ð¥ ) log2 ( ð¥ ) be the binar y entr opy func tion. Then, f or ð â ðŸ / ð , â ð †ðŸ(ð ð) †exp2 ( ð â ( ð ) ) †exp2 ( 2 ð ð log2 (1 ð) ) . Pr oof : F or a Bin ( ð , ð ) r andom v ariable ð , w e ha v e: 1 ⥠ð ( ð †ðŸ ) = â ð †ðŸ(ð ð) ðð( 1 â ð )ð â ð⥠â ð †ðŸ(ð ð) ððŸ( 1 â ð )ð â ᅵ... | https://arxiv.org/abs/2505.20607v1 |
t o see that ð â ( 0 , 1 / 2 ) and (2.3 ) holds f or all ðž †ð . The r esulting as y mpt otics f ollo w immediat ely . â¡ 2.2 C onditional Landscape Obstruction W e turn no w t o est ablishing the c entr al c onditional landscape obstruction of our ar gument. The idea is that f or an ð¥ â Σð depending on ð and a r ... | https://arxiv.org/abs/2505.20607v1 |
that â ð¥ â ð¥â²â2= 4 ð . Thus â ð¥ â ð¥â²â †2âð ð if and only if ð †ð ð < ð / 2 , so b y Lemma 2.2 , | ðµÎ£ ( ð¥ , ðð ) | = â ð †ð ð(ð ð) †exp2 ( 2 ð log2 ( 1 / ð ) ð ) . (2.7) T o bound the inner pr obabilit y under ðâ²âŒ1 â ð ð , fix an y ð¥â²â Σð and w rit e ðâ²= ð ð + â 1 â ð2 Ì ð f or ð â ... | https://arxiv.org/abs/2505.20607v1 |
exp2 ( â ðž + ð ( 1 ) ) , and w e c onc lude (2.5 ) as in the pr e v ious case . â¡ The f ollo w ing lemma sho w s a positiv e c orr elation pr opert y that enables us t o a v oid union-bound- ing o v er ð finding solutions t o c orr elat ed or r esampled pair s of inst anc es . Belo w , the set ð pla y s the r ole o... | https://arxiv.org/abs/2505.20607v1 |
) â ð ) , ð = ð ( ( ð , ð ) â ð , ( ðâ², ð ) â ð ) , ð ( ð ) = ð ( ( ð , ð ) â ð | ð ) , ð ( ð ) = ð ( ( ð , ð ) â ð , ( ðâ², ð ) â ð | ð ) . Lemma 2.5 sho w s that f or an y ð â Ωð , ð ( ð ) ⥠ð ( ð )2. Then, b y J ensen â s inequalit y , ð = ð [ ð ( ð ) ] ⥠ð [ ð ( ð )2] ⥠ð [ ð... | https://arxiv.org/abs/2505.20607v1 |
. â¡ Pr oof of Theor em 1.3 : Let ðsolve â ð ( ð ( ð ) â ð ( ðž ; ð ) ) be the pr obabilit y that ð solv es one inst anc e . By Lemma 2.5 , ððâ² âŒ1 â ð ð ( ðsolve ) ⥠ð2 solve . In addition, let ðcond â max ð¥ â Σð1 â ððâ² âŒ1 â ð ð ( ðcond ( ð¥ ) ) . ðunstable â 1 â ððâ² âŒ1 â ð ð ( ðstable ) , Set... | https://arxiv.org/abs/2505.20607v1 |
addition, define ðdiff â { ð â ðâ²} . Lemma 2.8 . F or ð¥ â ð ( ð ) , we have ðdiff â© ðsolve â© ðstable â© ðcond ( ð¥ ) = â
. Pr oof : This f ollo w s fr om Lemma 2. 7 , noting that the pr oof did not use that ð â ðâ² almost sur ely . â¡ As bef or e , our pr oof f ollo w s fr om sho w ing that f or appr opriat e ... | https://arxiv.org/abs/2505.20607v1 |
ð· ð =ð· ðlog2 (ð ð·) = ð ( 1 ) . Lik e w ise , f or (b ) log2ð ⪠ðž ⪠ð and ð· = ð ( ðž / log2( ð¶ ð / ðž ) ) , w e g et 16 ðunstable â²ð· log2 ( ð / ð· ) log2 ( ð¶ ð / ðž ) ðž As ð· is an upper bound on the maximum possible alg orithm degr ee , w e ma y incr ease ð· w ithout loss of g ener alit y in the ana... | https://arxiv.org/abs/2505.20607v1 |
appear , f ocusing on the L CD case . In the ne x t st ep t o w ar ds Theor em 1. 4 , w e sho w that our pr ec eding analy sis e x t ends t o ð ( 1 ) - dist anc e pertur bations of an L CD alg orithm, thank s t o the pr eser v ation of st abilit y . Thr oughout the belo w , fix a dist anc e ð = ð ( 1 ) . W e c onsid... | https://arxiv.org/abs/2505.20607v1 |
of ðunstable and ðcond as in (2.9 ) , ag ain r eplacing ð w ith Ì ðð . Thus , w e c hoose ð â log2 ( ð / ð· ) / ð , so that ð ( ðdiff ) â 1 . Additionally , c hoose ð as Lemma 2.3 , so that ðcond = ð ( 1 ) . It then suffic es t o sho w that ðunstable = ð ( 1 ) . T o see this , r ecall that when ðž = ð¿ ᅵ... | https://arxiv.org/abs/2505.20607v1 |
abo v e Theor em 1. 4 .) Lemma 2.10 . F ix ð¥ â ðð. Dr aw ð coin flips ðŒð¥ , ð ⌠Bern ( 2 ðð ( ð¥ ) ) as well as ð signs ðð ⌠Unif { ± 1 } , all mutuall y independent; define the r andom variable Ì ð¥ â Σð by Ì ð¥ð â ðð ðŒð¥ , ð + ( 1 â ðŒð¥ , ð ) ðððð ( ð¥ )ð . Then Ì ð¥ ⌠ðððððœ ( ð¥ ) . Pr o... | https://arxiv.org/abs/2505.20607v1 |
, the number of coor dinates Ì ð¥ is r esampled in di ver g es in pr obabilit y (i. e . e x ceeds an y fix ed ð < â with pr obabilit y 1 â ð ( 1 ) ). Pr oof : R ecall that f or ð¥ â [ 0 , 1 / 2 ] , w e ha v e log2 ( 1 â ð¥ ) = Î ( ð¥ ) . Thus , as eac h c oor dinat e of ð¥ is r ounded independently , w e can c omput ... | https://arxiv.org/abs/2505.20607v1 |
†2â ðž, â 2â ðžâ€ âš ð , ð¥ðœ â© â âš ð , ð¥ðœ ⩠†2â ðž. Multiply ing the lo w er equation b y â 1 and adding the r esulting inequalities giv es | âš ð , ð¥ðœ â© | †2â ðž. 19 Thus , finding pair s of distinct solutions w ithin dist anc e 2â ð implies finding a subset ðœ â [ ð ] of at most ð c oor dinat es and | ðœ |... | https://arxiv.org/abs/2505.20607v1 |
f or an y possible ð¥ = ð ( ð ) . N o w , let ðœ â [ ð ] denot e the set of the fir st ðŸ c oor dinat es t o be r esampled, so that ðŸ = | ðœ | , and c onsider ð ( Ì ð¥ â ð ( ðž ; ð ) | Ì ð¥ðœ ) , wher e w e fix the c oor dinat es out side of ðœ and let Ì ð¥ be unif ormly sampled fr om a ðŸ - dimensional subcube ... | https://arxiv.org/abs/2505.20607v1 |
fr om Phase Tr ansitions , â in 2008 4 9th A nnual IEEE S ymposium on F oundations of C omputer Science , Oct. 2008 , pp . 79 3â80 2. doi: 10 .1109 /F OCS .2008 .11 . [ A CR11] D . Ac hliopt as , A . C oja- O ghlan, and F . Ric ci- T er senghi, â On the solution-spac e g eometr y of r andom c onstr aint satisfaction pr... | https://arxiv.org/abs/2505.20607v1 |
C ommunications on Pur e and A pplied Mathematics , v ol. 7 6 , no . 10 , pp . 2410â24 7 3 , 20 23 . [Bar+19] B . Bar ak , S . Hopkins , J . K elner , P . K. K othari, A . Moitr a, and A . P ot ec hin, â A near ly tight sum- of-squar es lo w er bound f or the plant ed c lique pr oblem, â SIAM J ournal on C omputing , v... | https://arxiv.org/abs/2505.20607v1 |
. 2, pp . 217â240 , 2009 , doi: 10 .100 2 / r sa.20 25 5 . [Bor+09b] C. Bor g s , J . Cha y es , S . Mert ens , and C. N air , âPr oof of the Local REM C onjectur e f or N umber P artitioning . II. Gr o w ing Ener gy Scales , â R andom S truc tur es & Alg orithms , v ol. 34, no . 2, pp . 241â284, 2009 , doi: 10 .100 2 ... | https://arxiv.org/abs/2505.20607v1 |
eview Letter s , v ol. 4 5 , no . 2, pp . 79â8 2, J ul. 1980 , doi: 10 .110 3 /Ph y sR e vLett. 4 5 . 79 . [Der 81] B . Derrida, âR andom-Ener gy Model: An E x actly Solv able Model of Disor der ed S y st ems , â Ph ysical R eview B , v ol. 24, no . 5 , pp . 2613â26 26 , Sep . 1981, doi: 10 .110 3 /Ph y sR e vB .24.261... | https://arxiv.org/abs/2505.20607v1 |
and D . S . J ohnson, C omputer s and Intr ac tabilit y : A Guide to the Theor y of NP - C ompleteness . in A Series of Book s in the Mathematical Scienc es . N e w Y or k: W . H. F r eeman, 19 79 . [ GJK23] D . Gamarnik , A . J ag annath, and E. C. KızıldaÄ , âShatt ering in the Ising pur e ð -spin modelâ , arX i v p... | https://arxiv.org/abs/2505.20607v1 |
oblem â , SIAM J ournal on C omputing , v ol. 46 , no . 2, pp . 5 90â619 , 2017 . [ GW 00] I. Gent and T . W alsh, âPhase Tr ansitions and Annealed Theories: N umber P artitioning as a C ase Study , â Instituto C ultur a , J un. 2000 . [ GW 98] I. P . Gent and T . W alsh, â Analy sis of Heuristics f or N umber P artiti... | https://arxiv.org/abs/2505.20607v1 |
w w w . samuelbhopkins . c om / thesis .pdf [HS23] B . Huang and M. Sellk e , â Alg orithmic Thr eshold f or Multi-Species Spherical Spin Glasses , â arX i v :230 3 .12172 , 20 23 . [HS25a] B . Huang and M. Sellk e , â Tight Lipsc hit z Har dness f or Optimizing Mean F ield Spin Glasses , â C ommunications on Pur e and... | https://arxiv.org/abs/2505.20607v1 |
14th Innovations in Theor etical C omputer Science C onf er ence (IT CS 20 23 ) , 20 23 , p . 77 . [K AK19] A . M. Krieg er , D . Azriel, and A . K apelner , âN ear ly R andom Designs w ith Gr eatly Impr o v ed Balanc e , â Biometrik a , v ol. 106 , no . 3 , pp . 6 9 5â7 01, Sep . 2019 , doi: 10 .109 3 /biomet / asz0 2... | https://arxiv.org/abs/2505.20607v1 |
86 2 [K WB19] D . K unisk y , A . S . W ein, and A . S . Bandeir a, âN ot es on c omput ational har dness of h y pothesis t esting: Pr edictions using the lo w - degr ee lik elihood r atio , â in ISAA C C ongr ess (International Societ y f or A nal ysis, its A pplications and C omputation) , 2019 , pp . 1â50 . 23 [LKZ1... | https://arxiv.org/abs/2505.20607v1 |
e , pp . 125â160 , 2006 . [MH7 8] R. Mer kle and M. Hellman, âHiding Inf ormation and Signatur es in Tr apdoor Knapsac k s , â IEEE T r ansac tions on Inf ormation Theor y , v ol. 24, no . 5 , pp . 5 25â5 30 , Sep . 19 7 8 , doi: 10 .1109 /TIT .19 7 8 .105 5 9 2 7 . [MMZ 05] M. Mézar d, T . Mor a, and R. Zec c hina, â ... | https://arxiv.org/abs/2505.20607v1 |
o v . 198 2, pp . 14 5â15 2. doi: 10 .1109 /SF CS .198 2.5 . [TMR 20] P . T urner , R. Mek a, and P . Rig ollet, âBalancing Gaussian v ect or s in high dimension, â in C onf er ence on Learning Theor y , 20 20 , pp . 34 5 5â3486 . [T sa 9 2] L. -H. T sai, â As y mpt otic Analy sis of an Alg orithm f or Balanc ed P ar a... | https://arxiv.org/abs/2505.20607v1 |
arXiv:2505.20668v1 [math.ST] 27 May 2025Eigenstructure inference for high-dimensional covariance with generalized shrinkage inverse-Wishart prior Seongmin Kim1, Kwangmin Lee2, Sewon Park3, and Jaeyong Lee1 1Department of Statistics, Seoul National University 2Department of Big Data Convergence, Chonnam National Univers... | https://arxiv.org/abs/2505.20668v1 |
suggested sparse covariance estimation using thresholding methods. In the Bayesian lit erature,Banerjee and Ghosal (2015) suggested sparse precision estimation using the Gaussian graphical model. Lee et al.(2022) introduced a beta-mixture shrinkage prior for sparse cova riance and showed the posterior has nearly optima... | https://arxiv.org/abs/2505.20668v1 |
we directly compute the posterior expectation. Commonly, to investigate the asymptotic properties of the p osterior, researchers resort to general theorems on posterior convergence rates (e.g., Ghosal et al. (2000);Ghosal and van der Vaart (2007)). However, in this paper, we directly evaluate the posterio r expectation... | https://arxiv.org/abs/2505.20668v1 |
in high-dimensional settings, be comes even more severe. On the other hand, when b >1, the prior forces the eigenvalues to become nearly identic al. Accordingly, as proposed in Berger et al. (2020), we restrict bto the range [0 ,1] to avoid these undesirable behaviors. ConsiderthefollowingspectraldecompositionofΣ = UÎU... | https://arxiv.org/abs/2505.20668v1 |
Ã(¹|Î12,Îâ12,Î;H0)âetr(â1 2H1R¹Î12Îâ1ÎT 12RT ¹). 9 Let the spectral decomposition of Î 12Îâ1ÎT 12be Î12Îâ1ÎT 12= ï£cosÃâsinà sinÃcosÃ  ï£s10 0s2  ï£cosÃsinà âsinÃcosÃ , withs1> s2andÃâ(âà 2,à 2]. Then, the conditional density of ¹simpliï¬es to Ã(¹|Î12,Îâ12,Î;H0)âexp/parenleftbig ccos2(¹+Ã)/parenrightbig , wherec=â... | https://arxiv.org/abs/2505.20668v1 |
posterior convergence rates for eigenstruct ure, we assume the following conditions: A1. We consider high-dimensional settings where n/pâ0. A2. There exist positive constants c0andC0such that, for all n, C0> ÂŒ0,k+1>···> ÂŒ0,p> c0. A3. The klargest eigenvalues are suï¬ciently separated by a constant value¶0>0: ÂŒ0,jâÂŒ0,j+1... | https://arxiv.org/abs/2505.20668v1 |
may depend on nandp. Letϵ >0, and deï¬neÃ= min l<klog/parenleftbiggÂŒ0,l ÂŒ0,l+1/parenrightbigg . Suppose thatnp anzÂŒ0,k nÂŒ0,1à 2nϵ2andϵ{/radicalbiggnp an((nÃ)â1/2. Then, /integraldisplay (/uniontextL l=1Dϵ,l)cÃ(Î|Xn)(dÎ) =O/parenleftBig exp/parenleftBig âà 2nϵ2/parenrightBig ·/parenleftBig2ÂŒ0,1 ÂŒ0,k/parenrightBigkq/paren... | https://arxiv.org/abs/2505.20668v1 |
the convergence rate of the eigenvalues, while the second and third terms are attribute d to the convergence of the eigenvectors. Comparing the rate in ( 7) with the sample covariance rate in ( 8), we observe that the ï¬rst term in the sample covariance rate is larger. 17 4 Simulation Studies To evaluate the performance... | https://arxiv.org/abs/2505.20668v1 |
0.221 0.206 Ã2 0.419 0.443 0.466 0.427 0.673 0.428 Ã3 0.639 0.642 0.658 0.679 0.921 0.620 Table 2: Average errors (Err Ã) for estimated eigenvectors. Table1presents the average errors (Err ÂŒ), coverage probabilities (CP), and credible (or conï¬dence) interval length (IL) for the estimated spike d eigenvalues across diï¬e... | https://arxiv.org/abs/2505.20668v1 |
are relatively weak. Table3represents the average errors (Err ÂŒ), coverage probabilities (CP), and credible (or conï¬dence) interval length (IL) for the estimated spike d eigenvalues, across diï¬erent methods and values of n. The gSIW, SIW, and S-POET methods consistently outperform the sample covariance. In contrast, th... | https://arxiv.org/abs/2505.20668v1 |
k, the gSIW prior is applied, and the WAIC and IC p3are computed. WAIC and IC p3selectk= 7 and k= 9, respectively, while the GR method selects k= 1 as the optimal number of spiked eigenvalues. (a) Dimensionality reduction with k= 7 (WAIC). (b) Dimensionality reduction with k= 9 (ICp3). Figure 2: The images after dimens... | https://arxiv.org/abs/2505.20668v1 |
improving asymptotic bounds for sam ple eigenstructures in more general settings. Acknowledgements This work was supported by the National Research Foundation o f Korea (NRF) grant funded by the Korea government(MSIT) (No. NRF-2023R1A2C100305 0). 25 References Ahn, S. C. and Horenstein, A. R. (2013). Eigenvalue ratio t... | https://arxiv.org/abs/2505.20668v1 |
C. (2016). Nonparametric eigenvalue-regularized prec ision or covariance matrix estimator, AnnalsofStatistics 44(3): 928â953. Ledoit, O. and Wolf, M. (2004). A well-conditioned estimato r for large-dimensional co- variance matrices, Journalofmultivariate analysis88(2): 365â411. Ledoit, O. and Wolf, M. (2012). Nonlinear... | https://arxiv.org/abs/2505.20668v1 |
sum of two matrices AandB, whereA=1 nk/summationdisplay i=1ÂŒ0,iZiZT iandB=1 np/summationdisplay i=k+1ÂŒ0,iZiZT i. Lemma S1.2 (Asymptotic properties of eigenvalues of sample covariance) .Under model (1), the eigen- values of sample covariance satisfy the following properties for all suï¬ciently large n, ËÂŒj ÂŒ0,j=  ... | https://arxiv.org/abs/2505.20668v1 |
is given by D¿= 2/radicalbig min(n,pân). Lemma S1.5 (Probabilityofsubsetonorthogonalgroup) .Consider the following subset of the orthogonal groupO(p), deï¬ned as Bϵ=/braceleftbigg ÎâO(p) : inf Q1âO(n), Q2âO(pân)/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsing... | https://arxiv.org/abs/2505.20668v1 |
on Cϵ p/productdisplay i=n+1ci nf/parenleftBigh n/parenrightBigpân/bracketleftbigg 1+2ϵ2n (pân)hÂŒ0,1/bracketrightbiggpân , whereÂŽmax= max 1fjfkÂŽj, and for all suï¬ciently large n. Proof.For ÎâCϵ, the following inequality holds: (Îiiâ1)2+p/summationdisplay j=1 jÌž=iÎ2 ji< ϵ2, fori= 1,...,n. Sincep/summationdisplay j=1Î2 j... | https://arxiv.org/abs/2505.20668v1 |
the equality holds for all Î âBž: inf QâO(pân)||Î22âQ||2 F= inf QâO(pân)||DâQ||2 F = inf QâO(pân)pân/summationdisplay i=1[(/radicalBig ËÂŒiâqi)2+(1âq2 i)] =pân/summationdisplay i=1(/radicalBig ËÂŒiâ1)2 11 fmax ifpân/vextendsingle/vextendsingle/vextendsingleËÂŒiâ1/vextendsingle/vextendsingle/vextendsingle (/radicalbigËÂŒi+1... | https://arxiv.org/abs/2505.20668v1 |
ji(apâan) k+1ÃM(pânâp/summationtext i=n+1p/summationtext j=n+1Î2 ji)(ap+n 2â1) Mk(a1+n 2â1)+n/summationtext i=k+1p/summationtext j=n+1Î2 ji(an+n 2â1)/bracketrightBigg = sup Acϵ/bracketleftBigg 1 Kk/summationtext j=1p/summationtext i=k+1Î2 ji(anâak)+k/summationtext j=1p/summationtext i=n+1Î2 ji(apâak) kÃLn/summationtext... | https://arxiv.org/abs/2505.20668v1 |
ii)+p/summationdisplay j=1 jÌž=iÎ2 ji< ž2holds and it implies Î2 iig1âž2. Therefore, we obtain the upper bound of ( S4) as follows (S4)fsup Džk/productdisplay i=1/bracketleftbiggh n+Î2 iiËÂŒi+/summationdisplay j=1 jÌž=iÎ2 jiËÂŒj/bracketrightbiggai+n/2â1 17 fsup Džk/productdisplay i=1/bracketleftbiggh n+Î2 iiËÂŒi+(1âÎ2 ii)ËÂŒ... | https://arxiv.org/abs/2505.20668v1 |
non-negative diagonal elements, and ||PâS||Fgϵfor all permutation matrix P. Ifa1=···=ak, then the inequality holds sup Džk/producttext i=1/parenleftBigci n/parenrightBigai+n/2â1 inf Ežk/producttext i=1/parenleftBigci n/parenrightBigai+n/2â1âŒexp/parenleftBigg nž2ËÂŒ1 ËÂŒk/parenrightBigg exp/parenleftBigg nϵ2min i<klog/par... | https://arxiv.org/abs/2505.20668v1 |
iiâ1)2+(1âÎ2 ii)< ϵ2, it follows that Î2 ii>1âϵ2. Givenci n=h n+n/summationdisplay j=1Î2 jiËÂŒj,we obtain the bounds: ci nâ/bracketleftbigg (1âϵ2)ËÂŒi+h n,(1âϵ2)ËÂŒi+ϵ2ËÂŒ1+h n/bracketrightbigg ,fori= 1,...,n, ci nâ/bracketleftbiggh n, ϵ2ËÂŒ1+h n/bracketrightbigg ,fori=n+1,...,p. Under Î âDϵ, eachÂŒifollows an inverse gamma ... | https://arxiv.org/abs/2505.20668v1 |
Ã(Î,Î|Xn)(dÎ)(dÎ) = 1+ O/parenleftBig exp/parenleftBig âà 2nϵ2/parenrightBig ·/parenleftBig2ÂŒ0,1 ÂŒ0,k/parenrightBigkq/parenrightBig +O/parenleftBig/parenleftBignÂŒ0,k+p p/parenrightBigâϵ2an/parenrightBig , whereÃ= min l<klog/parenleftbiggÂŒ0,l ÂŒ0,l+1/parenrightbigg . Following the same bounding steps as in Lemma S1.16, w... | https://arxiv.org/abs/2505.20668v1 |
(dÎ). The last equality holds due to /vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle ï£Sl0 0Q2 âÎ/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/vextendsingle/v... | https://arxiv.org/abs/2505.20668v1 |
( S1.14), the upper bound of ( S18) is given by (S18)âŒexp/parenleftBigg n(ϵ+ϵ5)2ËÂŒ1 ËÂŒk/parenrightBigg exp/parenleftBigg n(ϵ4â(ϵ+ϵ5))2min i<klog/parenleftBiggËÂŒi ËÂŒi+1/parenrightBigg/parenrightBiggÃ/parenleftBig2ÂŒ0,1 ÂŒ0,k/parenrightBigkq âŒexp/parenleftbigg nϵ2ÂŒ0,1 ÂŒ0,k/parenrightbigg exp/parenleftbigg nϵ2 4min i<klog/p... | https://arxiv.org/abs/2505.20668v1 |
1â/integraldisplay (/uniontextL l=1Dϵ,l)c/parenleftBig/productdisplay ci/parenrightBigâaiân 2+1 (dÎ) /integraldisplay/parenleftBig/productdisplay ci/parenrightBigâaiân 2+1 (dÎ)/parenrightBigg ginf Dϵf(c)Ã/parenleftBig 1+O/parenleftBig exp/parenleftBig âà 2nϵ2/parenrightBig ·/parenleftBig2ÂŒ0,1 ÂŒ0,k/parenrightBigkq/paren... | https://arxiv.org/abs/2505.20668v1 |
for some constant ³0â[âC,C], we have t=¯dp n+³0/radicalbiggp n. Therefore, the posterior expectation simpliï¬es to: E/bracketleftBigÂŒiâÂŒ0,i ÂŒ0,i/vextendsingle/vextendsingleXn/bracketrightBig =1 ÂŒ0,i(³iâ³0)/radicalbiggp n+ÂŽi+1 ÂŒ0,ih n +O/parenleftBig ϵ2ÂŒ0,1 ÂŒ0,i+ÂŒ0,1 ÂŒ0,iexp/parenleftBig â» 2ϵ/parenrightBig +ÂŒ0,1 ÂŒ0,i/pa... | https://arxiv.org/abs/2505.20668v1 |
diï¬erence of eigenvectors) .For the spiked eigenvector matrix Î1, the following inequality holds on the set Dϵ: ||Î0,1âÎ1||2=O(dk)+Op(·k), where·k=1 ÂŒ0,k/radicalbiggp n+p n3/2ÂŒ0,k+1 n. Proof. ||Î0,1âÎ1||2f ||Î0,1âÎ1||2 F fk/summationdisplay i=1||Ã0,iâÃi||2 2 = 2k/summationdisplay i=1(1â/vextendsingle/vextendsingleÃT 0,... | https://arxiv.org/abs/2505.20668v1 |
0,i)·/parenleftbig O(dk)+Op(·k)/parenrightbig +k/summationdisplay i=1(ÂŒ0,iâËÂŒi)2/bracketrightBig +6/bracketleftBig 8/summationdisplay i>kÂŒ2 0,i+/summationdisplay i>k(ÂŒ0,iâËÂŒi)2/bracketrightBig . (S21) By Lemma S1.2, we obtain (ÂŒ0,iâËÂŒi)2=  O(p2 n2+ÂŒ2 0,i n1â2¶) fori= 1,...,k O(p2 n2) for i=k+1,...,n O(1) f... | https://arxiv.org/abs/2505.20668v1 |
arXiv:2505.20681v1 [stat.ME] 27 May 2025HYBRID BAYESIAN ESTIMATION IN THE ADDITIVE HAZARDS MODEL ÂŽAlvarez Enrique Ernesto1, Riddick Maximiliano Luis2 1Instituto de CÂŽ alculo, Universidad de Buenos Aires - CONICET Universidad Nacional de LujÂŽ an, Argentina mail: enriqueealvarez@fibertel.com.ar 2NUCOMPA and Departamendo ... | https://arxiv.org/abs/2505.20681v1 |
the previous ones by proposing a rescaling for the duration times themselves. I.e., Tâ=Tâ 0exp(Zâ²Î²),where Tâ 0âŒF0(·) is the baseline cumu- lative distribution function. Interestingly, for the corresponding hazard functions, this entails that λ(t,β) =λ0 texp(Zâ²Î²) exp(Zâ²Î²), (3) which is neither multiplicative nor addit... | https://arxiv.org/abs/2505.20681v1 |
hazard function itself, but not necessarily all the coefficients. In our context, there are two ways to accomplish that goal: (i) by adding the specific constraint that the estimated Ëλ(t) =Ëλ0(t) +βâ²zbe nonnegative and performing constrained inference; or ( ii) by using only positive covariates zk, either as given by ... | https://arxiv.org/abs/2505.20681v1 |
observations that belong to each grid interval, and calling ( zkj, ÎŽkj) to their corresponding covariate and censoring indicator, this yields Ln(β, λ0) = exp( âβâ²nX i=1tizi) exp( ânX i=1Î0(ti))mY j=1njY kj=1 aj+βâ²zkjÎŽkj(6) (7) Notice that the formula in Equation (6) above does not correspond to any stan- dard density... | https://arxiv.org/abs/2505.20681v1 |
Being a mixture of Gammas, the display above provides a tractable expression which we extensively exploit in the sequel. 2.1 Uninformative Priors 7 Without this convenient expression, several algorithms were presented in lit- erature with innovative adaptations of acceptance rejection sampling, Metropolis- Hastings and... | https://arxiv.org/abs/2505.20681v1 |
are currently under research. 3 The Hybrid Bayesian Method We attempt to develop a Bayesian method that achieves two goals, ( i) it disen- tangles estimation of βfrom the baseline hazard function λ0(·), as the latter is often treated as a nuisance in many applications, and ( ii) it generates estimators in closed form. ... | https://arxiv.org/abs/2505.20681v1 |
the mean or the mode of a multivariate normal distribution with mean vector m= (Vâ1 2V1) and covariance matrix is D=nâ1(Vâ1 2V3Vâ1 2). This entails that in a Bayesian context we could consider LY estimators as belonging to a posterior normal distribution for the Euclidean parameter with a flat (improper) prior. In this... | https://arxiv.org/abs/2505.20681v1 |
of (1 âα) coverage. The inter- val is of the form [ bl, bu], where 0 â€bl< bu<â. It is noteworthy that in Lin and Yingâs formulation, since the confidence intervals are based on the approximate normal distribution, they take the form ËβLY±z1âα/2ËÏ(ËβLY), which allows for a possibly negative lower endpoint. Here for the ... | https://arxiv.org/abs/2505.20681v1 |
order now to simplify notation, let us call d(j) k:=dk (sjâsjâ1)kÃÎ(c αj), cj:=Pnj kj=1(tkjâsjâ1) +mj(sjâsjâ1) (sjâsjâ1)+c. With that notation we express the posterior fÎ+ 0j|X,β(a+ 0) =PNj k=0d(j) k(a+ 0j)(k+c αjâ1)eâa+ 0jcj Râ ââPNj k=0d(j) k(a+ 0j)(k+c.αjâ1)eâa+ 0j.cjda+ 0 =PNj k=0d(j) k ck jÎ(k+c αj)fG(k+c αj,c... | https://arxiv.org/abs/2505.20681v1 |
a single covariate with regression parameter β= 0.5, (ii) Censoring variable Cwith an Exponential distribution with mean 2, ( iii) Covariate ZâŒÏ2 1, (iv) sample sizes n= 100 or 500, and ( v)R= 1000 replicates. Simulations for the regression parameter β.The results are presented in Tables (1) and (2). We observe that in... | https://arxiv.org/abs/2505.20681v1 |
) (0.1024 ) (0.1030 ) (0.1033 ) (0.1035 ) (0.1035 ) (0.1036 ) 2 0.6543 0.5419 0.5264 0.5186 0.5138 0.5122 0.5106 (0.0982 ) (0.1024 ) (0.1030 ) (0.1033 ) (0.1035 ) (0.1035 ) (0.1036 ) 10 1.4375 0.7128 0.6128 0.5620 0.5312 0.5209 0.5107 (0.0982 ) (0.1024 ) (0.1030 ) (0.1033 ) (0.1035 ) (0.1035 ) (0.1036 ) Table 2: Simula... | https://arxiv.org/abs/2505.20681v1 |
2.6005 log(EXP+1) 1.7172 1.7081 1.7172 Table 5: (Results are multiplied by 103) The results are presented in Table (5), where we visualize the impact of the choice of the hyperparameters on the final estimates. Those results show the versatility of our proposed Hybrid Bayesian method, which can be calibrated to give th... | https://arxiv.org/abs/2505.20681v1 |
& Sons. Klein, J. P. and Moeschberger, M. L. (2006). Survival analysis: techniques for censored and truncated data . Springer Science & Business Media. 20 Lawless, J. F. (2003). Event history analysis and longitudinal surveys. Analysis of Survey data , 221-243. Lin, D. Y. and Ying, Z. (1994). Semiparametric Analysis of... | https://arxiv.org/abs/2505.20681v1 |
arXiv:2505.20708v1 [econ.TH] 27 May 2025Berk-Nash Rationalizabilityâ Ignacio Esponda Demian Pouzo UC Santa Barbara UC Berkeley May 28, 2025 Abstract We introduce BerkâNash rationalizability , a new solution concept for misspeciï¬ed learning environments. It parallels rationalizability in games and captures all actions t... | https://arxiv.org/abs/2505.20708v1 |
environments or rely on paramet ric assumptions such as Gaussian signals or binary states. Examples include Nyarko(1991),Fudenberg, Romanyuk and Strack (2017), Heidhues, KË oszegi and Strack (2018),Heidhues, KË oszegi and Strack (2021),Bohren and Hauser (2021), and He(2022) among many others. 3Limit actions are deï¬ned ... | https://arxiv.org/abs/2505.20708v1 |
space A, a space of observable consequences Y, and a consequence function that maps actions to probability distributions over consequences, denoted by Q:AââY. The agent does not necessarily knowQbut possesses a parametric model of it, represented as QΞ:AââY, where the model parameter Ξbelongs to a parameter space Î. Th... | https://arxiv.org/abs/2505.20708v1 |
distribution Q(· |a) corresponds to a normal distribution with mean ( αâ+a)Ξâand the same variance. These distributions admit densities with respect to the Lebesgue measure that vary co ntinuously in aandΞ, and they satisfy the uniform integrability condition with a quadratic e nvelope. The agentâs payoï¬ function is Ï(... | https://arxiv.org/abs/2505.20708v1 |
about consequences arises f rom actions drawn from the setA, then the models that provide the best ï¬t are those that minimize KL divergence for some action distribution supported on A. Consequently, the agent will follow actions that are optimal for beliefs that assign probability one to these best-ï¬t models. Example (... | https://arxiv.org/abs/2505.20708v1 |
ytdrawn from the distribution Q(· |at), â¢And updates beliefs via Bayesâ rule: µt+1=Bay(at,yt,µt), 6EP also considered mixed actions. Every action in the support of an e quilibrium mixed action is ratio- nalizable. 7EP consider forward-looking agents under a conditionâweak identiï¬ cationâthat guarantees incentives to ex... | https://arxiv.org/abs/2505.20708v1 |
|a). The marginal distribution of PoverAâis denoted by PAâ. An action aâAis called a limit action of the sequence aâ= (a1,a2,...) if there exists a subsequence ( atk)ksuch that atkâaaskâ â. Equivalently, ais a limit action if, for every open neighborhood UâAofa, there are inï¬nitely many times tâNsuch that atâU. WhenAis... | https://arxiv.org/abs/2505.20708v1 |
and Î is nonempty-valued and upper hemicontinuous, eac h set Bkis nonempty and compact. The inï¬nite intersection of nested, none mpty compact sets is nonempty, so Bis nonempty. This typeofcharacterizationisstandardwhen rationalizabilityisdeï¬ nedasclosureunder a set-valued operator. Just as in other familiar settingsâsu... | https://arxiv.org/abs/2505.20708v1 |
rationalizable actions. The limits also satisfy T(aâ min) =aâ max, T(aâ max) =aâ min, 12 so they form a 2-cycle of Tand are ï¬xed points of T2. IfT2has a unique ï¬xed point, then it must also be a ï¬xed point of T, and the limit is a singleton. In that case, rationalizability coincides with equilibrium. If T2has multiple ... | https://arxiv.org/abs/2505.20708v1 |
actions, denoted aSandaL, respectively. These actions are also the smallest and largest Berk-Nash equilibrium actions. They can be cons tructed as the limits of the monotone sequences: ak+1 S=a(Ξ(ak S)), ak+1 L= ¯a(¯Ξ(ak L)), starting from a0 S= minAanda0 L= maxA. The limits aS= limkââak SandaL= limkââak L are ï¬xed poi... | https://arxiv.org/abs/2505.20708v1 |
whereËB0=AandËBk+1=T(ËBk), whereT(·) = ËaâŠËΞ(·). This characterization is convenient because the operator Î is deï¬n ed over mixed actions and mixed beliefs, which can be diï¬cult to work with directly. In contra st, the operator 15 Tin Proposition 3allows us to focus entirely on degenerate actions and beliefs, while st ... | https://arxiv.org/abs/2505.20708v1 |
the fact that there is a function gaâL2(Y,R,Q(· |a)) such that supΞâ²âO(Ξ,ε)(g(Ξâ²,y,x))2â€(ga(y))2, whereg(Ξ,y,x) := log( q(y|a)/qΞ(y|a)) and O(Ξ,ε) :={Ξâ²:||Ξâ²âΞ||< ε}. In our case, we need a function Gthat does not depend on a; hence our assumption (v). In Step 2 of their proof, they conclude that, for each ΞâÎ, Î ÎŽ(a) ... | https://arxiv.org/abs/2505.20708v1 |
Consider Ξ/\e}atio\slashâ€Â¯Îž(ah). Since¯Ξ(xh) is the largest minimizer of K(·,xh) andΞâšÂ¯Îž(ah)> ¯Ξ(ah), thenK(¯Ξ(ah),ah)< K(ΞâšÂ¯Îž(ah),ah). SinceâKis single crossing in ( Ξ,a), this implies K(¯Ξ(ah),a)< K(ΞâšÂ¯Îž(ah),a) for all aâ[al,ah]. Since âKis quasi-supermodular in Ξ, this implies K(Ξâ§Â¯Îž(xh),a)< K(Ξ,a) for all aâ[al,ah]... | https://arxiv.org/abs/2505.20708v1 |
similar if a < a). Strict quasiconcavity of U(·,Ξ) implies that, for all ΞâËΞ(A), U(a,Ξ)< U(¯a,Ξ)â€U(Ëa(Ξ),Ξ). Therefore, for any µââËA, /integraldisplay U(a,Ξ)µ(dΞ)</integraldisplay U(¯a,Ξ)µ(dΞ), implying that a /âF(âËΞ(A)) =F(â(âªÏââAÎm(Ï))), where the equality follows from equa- tion (16). SinceF(â(âªÏââAÎm(Ï)))âÎ(A), ... | https://arxiv.org/abs/2505.20708v1 |
arXiv:2505.20946v1 [math.ST] 27 May 2025Almost Unbiased Liu Estimator in Bell Regression Model: Theory and Application Caner Tanıž sâ and Yasin Asarâ¡ â Department of Statistics, C žankırı Karatekin University e-mail: canertanis@karatekin.edu.tr â¡Department of Mathematics and Computer Sciences, Necmettin Erbakan Universit... | https://arxiv.org/abs/2505.20946v1 |
devel- oped to ï¬t the speciï¬c needs of these regression models. More recent studies have proposed a novel Liu estimator for Bell regression, with performance e valuations conducted through simula- tion studies. Comparative analyses between ridge andLiu es timators have also beenundertaken, particularly in the context o... | https://arxiv.org/abs/2505.20946v1 |
distribution. â¢The Bell distribution is a member of the one-parameter expon ential distributions. â¢The Bell distribution is unimodal. â¢The Poisson distribution does not follow the Bell family of d istributions. But if the pa- rameter has a small value, the Bell distribution approximat es to the Poisson distribution. â¢T... | https://arxiv.org/abs/2505.20946v1 |
solution of U/parenleftBig /hatwideβ/parenrightBig =0p, where 0prefers a p-dimensional vector of zeros. Regrettably, the maximum likelihood estimator /hatwideβlacks a closed-form solution, necessitating its numerical computation. For instance, the NewtonâRaphs on iterative method is one possible approach. Alternatively... | https://arxiv.org/abs/2505.20946v1 |
d in the Bell regression model. 6 In the Bell regression, the AULE is /hatwideβAULE=/parenleftBig Iâ(1âd)2(F+I)â2/parenrightBig /hatwideβMLE. The covariance matrix and bias vector of the AULE are Cov/parenleftBig /hatwideβAULE/parenrightBig =Cov/parenleftBig Iâ(1âd)2(F+I)â2/hatwideβMLE/parenrightBig =/parenleftBig Iâ(1... | https://arxiv.org/abs/2505.20946v1 |
λj+d/parenrightbig2/parenleftbig λj+2âd/parenrightbig2 λj/parenleftbig λj+1/parenrightbig4 =p/summationdisplay j=1/parenleftbig λj+1/parenrightbig4â/parenleftbig λj+d/parenrightbig2/parenleftbig λj+2âd/parenrightbig2 λj/parenleftbig λj+1/parenrightbig4. The diï¬erence between the variances of MLE and AULE is positiv e f... | https://arxiv.org/abs/2505.20946v1 |
5.2482 5.1354 5.3143 200 0.9 15.4715 4.7503 4.7207 4.5908 4.7601 400 0.9 11.7297 3.0397 3.0136 2.9411 3.0421 100 0.95 17.0654 5.5808 5.5327 5.5002 5.5956 200 0.95 15.6238 4.8431 4.8150 4.7800 4.8511 400 0.95 10.3919 2.5382 2.5024 2.4961 2.5321 Table 5: Simulated MSE values when p= 8 nÏMLE LE AULE(d1)AULE(d2)AULE(d3) 10... | https://arxiv.org/abs/2505.20946v1 |
data y(response variable) the number of defects per laminated pla stic plywood area x1 volumetric shrinkage x2 assembly time x3 wood density x4 drying temperature The design matrix is centered and standardized so that Xâ€Xis in the correlation form before obtaining the estimators. A Bell regression model without i nterc... | https://arxiv.org/abs/2505.20946v1 |
1.0 dSBEstimators AULE LE Figure 4: MSEs and SBs of the estimators for â1< d <1 200400600 0.00 0.25 0.50 0.75 1.00 dMSEEstimators AULE LE MLE 0204060 0.00 0.25 0.50 0.75 1.00 dSBEstimators AULE LE Figure 5: MSEs and SBs of the estimators for 0 < d <1 6 Conclusion In this paper, we introduced a new biased estimator call... | https://arxiv.org/abs/2505.20946v1 |
Amin, M., Qasim, M., Afzal, S., Naveed, K. (2022). New ridgee stimators in theinverse Gaussian regression: Monte Carlo simulation and application to chem ical data. Communications in StatisticsâSimulation and Computation, 51(10), 6170â618 7. Amin, M., Akram, M. N., Majid, A. (2023). On the estimation of Bell regression... | https://arxiv.org/abs/2505.20946v1 |
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