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Journal articles on the topic 'Non zero'

Author: Grafiati

Published: 5 June 2025

Last updated: 16 July 2025

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1

Li, Bo, Lin Chen, and Heng Fan. "Non-zero total correlation means non-zero quantum correlation." Physics Letters A 378, no. 18-19 (2014): 1249–53. http://dx.doi.org/10.1016/j.physleta.2014.02.036.

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2

Schmidt, Christian. "QCD thermodynamics at zero and non-zero density." Nuclear Physics A 820, no. 1-4 (2009): 41c—48c. http://dx.doi.org/10.1016/j.nuclphysa.2009.01.017.

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3

Cococcioni, Marco, Lorenzo Fiaschi, and Luca Lambertini. "Non-Archimedean zero-sum games." Journal of Computational and Applied Mathematics 393 (September 2021): 113483. http://dx.doi.org/10.1016/j.cam.2021.113483.

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4

Schwartz, Hannah R. "Duals of non-zero square." Mathematical Research Letters 29, no. 1 (2022): 275–84. http://dx.doi.org/10.4310/mrl.2022.v29.n1.a8.

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5

Hatzenbuhler, J., and D. A. Mattson. "Non-scattered zero-dimensional remainders." Rocky Mountain Journal of Mathematics 18, no. 3 (1988): 635–44. http://dx.doi.org/10.1216/rmj-1988-18-3-635.

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6

Grishukhin, V. P. "Parallelotopes of non-zero width." Sbornik: Mathematics 195, no. 5 (2004): 669–86. http://dx.doi.org/10.1070/sm2004v195n05abeh000821.

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7

Soskin, S. M., and D. G. Luchinsky. "Zero-dispersion non-linear resonance." Il Nuovo Cimento D 17, no. 7-8 (1995): 915–24. http://dx.doi.org/10.1007/bf02451849.

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8

Bytsenko, A. A., and S. D. Odintsov. "Supermembranes at Non-Zero Temperature." Fortschritte der Physik 41, no. 3 (1993): 233–60. http://dx.doi.org/10.1002/prop.19930410306.

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9

Bytsenko, A. A., and S. D. Odintsov. "Supermembranes at Non-Zero Temperature." Fortschritte der Physik/Progress of Physics 41, no. 3 (1993): 233–60. http://dx.doi.org/10.1002/prop.2190410306.

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10

Zamani, Amirreza, and Mikael Skoglund. "Variable-Length Coding with Zero and Non-Zero Privacy Leakage." Entropy 27, no. 2 (2025): 124. https://doi.org/10.3390/e27020124.

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A private compression design problem is studied, where an encoder observes useful data Y, wishes to compress them using variable-length code, and communicates them through an unsecured channel. Since Y are correlated with the private attribute X, the encoder uses a private compression mechanism to design an encoded message C and sends it over the channel. An adversary is assumed to have access to the output of the encoder, i.e., C, and tries to estimate X. Furthermore, it is assumed that both encoder and decoder have access to a shared secret key W. In this work, the design goal is to encode message C with the minimum possible average length that satisfies certain privacy constraints. We consider two scenarios: 1. zero privacy leakage, i.e., perfect privacy (secrecy); 2. non-zero privacy leakage, i.e., non-perfect privacy constraint. Considering the perfect privacy scenario, we first study two different privacy mechanism design problems and find upper bounds on the entropy of the optimizers by solving a linear program. We use the obtained optimizers to design C. In the two cases, we strengthen the existing bounds: 1. |X|≥|Y|; 2. The realization of (X,Y) follows a specific joint distribution. In particular, considering the second case, we use two-part construction coding to achieve the upper bounds. Furthermore, in a numerical example, we study the obtained bounds and show that they can improve existing results. Finally, we strengthen the obtained bounds using the minimum entropy coupling concept and a greedy entropy-based algorithm. Considering the non-perfect privacy scenario, we find upper and lower bounds on the average length of the encoded message using different privacy metrics and study them in special cases. For achievability, we use two-part construction coding and extended versions of the functional representation lemma. Lastly, in an example, we show that the bounds can be asymptotically tight.

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11

Müller, Ruth, and Sarah Maria Schönbauer. "Zero Waste––Zero Justice?" Engaging Science, Technology, and Society 6 (November 2, 2020): 416. http://dx.doi.org/10.17351/ests2020.649.

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Plastic is slowly covering the earth, accumulating in oceans, soil, air, and human and non-human bodies. In the face of this catastrophe, zero waste activists call upon us for action, detailing, how we, too, can change our lifestyle to eliminate plastic waste and save the planet. Yet, who it is that is called upon, who speaks, and whose voices and lived realities might be ignored? In this contribution, we explore the social politics of the zero waste movement. This leads us to ponder: might popular environmental movements that relegate social justice to the back seat ultimately do more harm than good?

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12

Mary Mathew, Vrinda, and Sudev Naduvath. "Coloring of Non-Zero Component Graphs." Proyecciones (Antofagasta) 43, no. 4 (2024): 883–98. http://dx.doi.org/10.22199/issn.0717-6279-5962.

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The non-zero component graph of finite dimensional vector space V over a finite field F is the graph G(Vα)= (V,E), where vertices of G(Vα) are the non-zero vectors in V, two of which are adjacent if they share at least one basis vector with non-zero coefficient in their basic representation. In this paper, we study the various types of colorings of non-zero component graph.

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13

AGUDOV, N. V., and A. V. SAFONOV. "RELAXATION TIMES IN SYSTEMS WITH ZERO AND NON-ZERO STATIONARY FLOW." Fluctuation and Noise Letters 03, no. 02 (2003): L107—L112. http://dx.doi.org/10.1142/s0219477503001166.

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We examine the kinetics of relaxation processes in dynamical models with the fixed number of Brownian particles and with the constant source of the particles. The former evolves to the zero equilibrium distribution, while the latter develops to the stationary state with non-equilibrium distribution and non-zero stationary flow. We show that the relaxation times in the both systems coincide. This is valid for an arbitrary noise intensity and shape of potential profile. In addition we propose to modify the well-known Kramers' approach for the determination of relaxation time. The modified approach is valid for an arbitrary height of potential barriers.

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14

Chabriel, Gilles, and Jean Barrere. "Non-Symmetrical Joint Zero-Diagonalization and MIMO Zero-Division Multiple Access." IEEE Transactions on Signal Processing 59, no. 5 (2011): 2296–307. http://dx.doi.org/10.1109/tsp.2011.2106122.

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15

Bazavov, A., H. T. Ding, P. Hegde, et al. "Chiral crossover in QCD at zero and non-zero chemical potentials." Physics Letters B 795 (August 2019): 15–21. http://dx.doi.org/10.1016/j.physletb.2019.05.013.

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16

Di Giacomo, A., E. Meggiolaro, and H. Panagopoulos. "Field strength correlators in QCD at zero and non-zero temperature." Nuclear Physics B - Proceedings Supplements 54, no. 1-2 (1997): 343–47. http://dx.doi.org/10.1016/s0920-5632(97)00065-0.

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17

Farwig, Reinhard, and Hermann Sohr. "The stationary and non-stationary stokes system in exterior domains with non-zero divergence and non-zero boundary values." Mathematical Methods in the Applied Sciences 17, no. 4 (1994): 269–91. http://dx.doi.org/10.1002/mma.1670170405.

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18

Petreczky, P. "Lattice QCD at non-zero temperature." Journal of Physics G: Nuclear and Particle Physics 39, no. 9 (2012): 093002. http://dx.doi.org/10.1088/0954-3899/39/9/093002.

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19

de Vega, H. J., and L. N. Lipatov. "Reggeon Dynamics at non-zero Temperature." Nuclear Physics B - Proceedings Supplements 146 (September 2005): 123–25. http://dx.doi.org/10.1016/j.nuclphysbps.2005.02.075.

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20

Akhmedov, Anar. "Surface bundles with non-zero signature." Topology and its Applications 154, no. 11 (2007): 2235–40. http://dx.doi.org/10.1016/j.topol.2007.02.009.

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21

Chalauri, Giga, Vakhtang Laluashvili, and Koba Gelashvili. "Jagged non-zero submatrix data structure." Transactions of A. Razmadze Mathematical Institute 172, no. 1 (2018): 7–14. http://dx.doi.org/10.1016/j.trmi.2017.10.002.

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22

Alford, Mark, Katherine Benson, Sidney Coleman, John March-Russell, and Frank Wilczek. "Zero modes of non-abelian vortices." Nuclear Physics B 349, no. 2 (1991): 414–38. http://dx.doi.org/10.1016/0550-3213(91)90331-q.

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23

Urban, Martin, and Petr Kulhánek. "z-pinch with non zero helicity." Czechoslovak Journal of Physics 46, no. 11 (1996): 1093–98. http://dx.doi.org/10.1007/bf01690038.

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24

Dyakonov, D. I., and A. D. Mirlin. "Instanton vacuum at non-zero temperatures." Physics Letters B 203, no. 3 (1988): 299–304. http://dx.doi.org/10.1016/0370-2693(88)90557-6.

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25

Holm, Ruurik. "Non-zero probabilities for universal generalizations." Synthese 190, no. 18 (2013): 4001–7. http://dx.doi.org/10.1007/s11229-013-0244-x.

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26

Xu, Baogen, Mengmeng Zheng, and Ting Lan. "On Non-Zero Vertex Signed Domination." Symmetry 15, no. 3 (2023): 741. http://dx.doi.org/10.3390/sym15030741.

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For a graph G=(V,E) and a function f:V→{−1,+1}, if S⊆V then we write f(S)=∑v∈Sf(v). A function f is said to be a non-zero vertex signed dominating function (for short, NVSDF) of G if f(N[v])=0 holds for every vertex v in G, and the non-zero vertex signed domination number of G is defined as γsb(G)=max{f(V)|f is an NVSDF of G}. In this paper, the novel concept of the non-zero vertex signed domination for graphs is introduced. There is also a special symmetry concept in graphs. Some upper bounds of the non-zero vertex signed domination number of a graph are given. The exact value of γsb(G) for several special classes of graphs is determined. Finally, we pose some open problems.

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27

Drăgulete, Oana, and Liviu Ornea. "Non-zero contact and Sasakian reduction." Differential Geometry and its Applications 24, no. 3 (2006): 260–70. http://dx.doi.org/10.1016/j.difgeo.2005.09.003.

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28

Aksenov, V. P., V. V. Dudorov, G. A. Filimonov, V. V. Kolosov, and V. Yu Venediktov. "Vortex beams with zero orbital angular momentum and non-zero topological charge." Optics & Laser Technology 104 (August 2018): 159–63. http://dx.doi.org/10.1016/j.optlastec.2018.02.022.

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29

Portela, Maria Conceição A. Silva, and Emmanuel Thanassoulis. "Zero weights and non-zero slacks: Different solutions to the same problem." Annals of Operations Research 145, no. 1 (2006): 129–47. http://dx.doi.org/10.1007/s10479-006-0029-4.

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30

DĂSCĂLESCU, S., C. NĂSTĂSESCU, and B. TORRECILLAS. "INVOLUTORY HOPF ALGEBRAS WITH NON-ZERO INTEGRALS." Bulletin of the London Mathematical Society 34, no. 1 (2002): 33–36. http://dx.doi.org/10.1112/s0024609301008682.

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31

Vázquez, Carlos Manuel. "Less Than Zero?" American Journal of International Law 102, no. 3 (2008): 563–72. http://dx.doi.org/10.2307/20456644.

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Medellín v. Texas is the first case in which the Supreme Court has denied a treaty-based claim solely on the ground that the treaty relied upon was non-self-executing. In Foster v. Neilson, the only other case in which the Court had denied relief on this ground, the Court offered its view that the treaty was non-self-executing as an alternative ground for denying relief. The Court soon thereafter disavowed its conclusion that the treaty involved in Foster was non-selfexecuting, and, in the intervening years, it repeatedly declined invitations to deny relief on this or related grounds. Many observers (including me) thought that the Court would again skirt a ruling on non-self-execution in Medellín because the president had issued a memorandum ordering compliance with the judgment of the International Court of Justice (ICJ) in Avena. After all, the Court in American Insurance Ass’n v. Garamendi had recently struck down a California law on the ground that it conflicted with a “policy” reflected in certain sole executive agreements. The president in Medellín seemed to be standing on stronger ground, as he was insisting that state law give way to an obligation imposed by a treaty that had received the consent of the Senate and was accordingly the supreme law of the land. But the Court defied this expectation, with potentially regrettable results for the law of treaties.

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32

Majumder, S., and A. Dam. "On certain non-linear differential monomial sharing non-zero polynomial." Ukrains’kyi Matematychnyi Zhurnal 73, no. 2 (2021): 201–21. http://dx.doi.org/10.37863/umzh.v73i2.99.

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UDC 517.5 With the idea of normal family we study the uniqueness of meromorphic functions and when and share two values, where and is a polynomial. The obtained result significantly improves and generalizes the result in [A. Banerjee, S. Majumder, <em>On certain non-linear differential polynomial sharing a non-zero polynomial</em>, Bol. Soc. Mat. Mex. (2016),https://doi.org/10.1007/s40590-016-0156-0].

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33

Majumder, Sujoy. "Certain non-linear differential polynomials sharing a non zero polynomial." Acta Universitatis Sapientiae, Mathematica 7, no. 1 (2015): 35–66. http://dx.doi.org/10.1515/ausm-2015-0004.

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Abstract In this paper with the notion of weighted sharing of values we study the uniqueness of nonlinear differential polynomials of meromorphic functions sharing a nonzero polynomial and obtain two results which improves and generalizes the results due to L. Liu [Uniqueness of meromorphic functions and differential polynomials, Comput. Math. Appl., 56 (2008), 3236-3245.] and P. Sahoo [Uniqueness and weighted value sharing of meromorphic functions, Applied. Math. E-Notes., 11 (2011), 23-32.].

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34

Acosta, J. Alberto, Alfredo Aranda, Manuel A. Buen-Abad та Alma D. Rojas. "Non-diagonal charged lepton mass matrix and non-zero θ13". Physics Letters B 718, № 4-5 (2013): 1413–20. http://dx.doi.org/10.1016/j.physletb.2012.12.038.

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35

Bettin, Sandro, Chantal David, and Christophe Delaunay. "Non-isotrivial elliptic surfaces with non-zero average root number." Journal of Number Theory 191 (October 2018): 1–84. http://dx.doi.org/10.1016/j.jnt.2018.03.007.

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36

Durga Prasad, M. V., and P. C. Sreenivas. "Vector Valued Non Zero Sum Games and Non Linear Programming." OPSEARCH 34, no. 3 (1997): 180–85. http://dx.doi.org/10.1007/bf03398522.

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37

Kish, Laszlo B., Gunnar A. Niklasson, and Claes-Göran Granqvist. "Zero Thermal Noise in Resistors at Zero Temperature." Fluctuation and Noise Letters 15, no. 03 (2016): 1640001. http://dx.doi.org/10.1142/s0219477516400010.

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The bandwidth of transistors in logic devices approaches the quantum limit, where Johnson noise and associated error rates are supposed to be strongly enhanced. However, the related theory — asserting a temperature-independent quantum zero-point (ZP) contribution to Johnson noise, which dominates the quantum regime — is controversial and resolution of the controversy is essential to determine the real error rate and fundamental energy dissipation limits of logic gates in the quantum limit. The Callen–Welton formula (fluctuation–dissipation theorem) of voltage and current noise for a resistance is the sum of Nyquist’s classical Johnson noise equation and a quantum ZP term with a power density spectrum proportional to frequency and independent of temperature. The classical Johnson–Nyquist formula vanishes at the approach of zero temperature, but the quantum ZP term still predicts non-zero noise voltage and current. Here, we show that this noise cannot be reconciled with the Fermi–Dirac distribution, which defines the thermodynamics of electrons according to quantum-statistical physics. Consequently, Johnson noise must be nil at zero temperature, and non-zero noise found for certain experimental arrangements may be a measurement artifact, such as the one mentioned in Kleen’s uncertainty relation argument.

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38

Zhuravlov, V. "Non-standard sequences." Matematychni Studii 63, no. 1 (2025): 14–20. https://doi.org/10.30970/ms.63.1.14-20.

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The paper shows the existence of a previously unknown relationship between the theory of monoids and category theory. A non-standard mathematical method based on terms from non-standard (not always existing) sequences is proposed. In the article in particular are proved the following statement: Every category is a complete model of some monoid with an associative zero. Conversely, any such monoid completely models some category. Category theory is logically equivalent to the theory of monoids with an associative zero. Both are non-essential extensions of each other. (Theorem 1)

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39

Zhou, Xiao, Yu Kang, Tingting Zhang, and Xingang Mou. "M-Array Based on Non-Zero Maps." IEEE Access 9 (2021): 58467–77. http://dx.doi.org/10.1109/access.2021.3071877.

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40

Tian, Wei-zhong, Ting-ting Liu, and Yao-ting Yang. "Zero-inflated non-central negative binomial distribution." Applied Mathematics-A Journal of Chinese Universities 37, no. 2 (2022): 187–98. http://dx.doi.org/10.1007/s11766-022-4070-0.

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41

Tuganbaev, Timur, and Kenya Honda. "Non‐zero‐sum microbiome immune system interactions." European Journal of Immunology 51, no. 9 (2021): 2120–36. http://dx.doi.org/10.1002/eji.202049065.

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42

Lombardo, M. P. "QCD at non-zero density: lattice results." Journal of Physics G: Nuclear and Particle Physics 35, no. 10 (2008): 104019. http://dx.doi.org/10.1088/0954-3899/35/10/104019.

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43

Avilés-Casco, Alejandro Vaquero, Carleton DeTar, Daping Du, et al. "B → D*lv at non-zero recoil." EPJ Web of Conferences 175 (2018): 13003. http://dx.doi.org/10.1051/epjconf/201817513003.

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We present preliminary results from our analysis of the form factors for the B → D*lv decay at non-zero recoil. Our analysis includes 15 MILC asqtad ensembles with Nf = 2 + 1 flavors of sea quarks and lattice spacings ranging from a ≈ 0.15 fm down to 0.045 fm. The valence light quarks employ the asqtad action, whereas the heavy quarks are treated using the Fermilab action. We conclude with a discussion of future plans and phenomenological implications. When combined with experimental measurements of the decay rate, our calculation will enable a determination of the CKM matrix element |Vcb|.

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44

Murat, M., and D. Szynal. "Non–zero inflated modified power series distributions." Communications in Statistics - Theory and Methods 27, no. 12 (1998): 3047–64. http://dx.doi.org/10.1080/03610929808832272.

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45

Bergman, L. M., and I. N. Fokin. "On separable non-cooperative zero-sum games." Optimization 44, no. 1 (1998): 69–84. http://dx.doi.org/10.1080/02331939808844400.

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46

Cao, Yongluo. "Non-zero Lyapunov exponents and uniform hyperbolicity." Nonlinearity 16, no. 4 (2003): 1473–79. http://dx.doi.org/10.1088/0951-7715/16/4/316.

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47

Parra, Jorge, Irene Olivares, Antoine Brimont, and Pablo Sanchis. "Non-volatile epsilon-near-zero readout memory." Optics Letters 44, no. 16 (2019): 3932. http://dx.doi.org/10.1364/ol.44.003932.

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48

BEHBOODI, M., R. BEYRANVAND, and H. KHABAZIAN. "STRONG ZERO-DIVISORS OF NON-COMMUTATIVE RINGS." Journal of Algebra and Its Applications 08, no. 04 (2009): 565–80. http://dx.doi.org/10.1142/s0219498809003540.

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We introduce the set S(R) of "strong zero-divisors" in a ring R and prove that: if S(R) is finite, then R is either finite or a prime ring. When certain sets of ideals have ACC or DCC, we show that either S(R) = R or S(R) is a union of prime ideals each of which is a left or a right annihilator of a cyclic ideal. This is a finite union when R is a Noetherian ring. For a ring R with |S(R)| = p, a prime number, we characterize R for S(R) to be an ideal. Moreover R is completely characterized when R is a ring with identity and S(R) is an ideal with p2 elements. We then consider rings R for which S(R)= Z(R), the set of zero-divisors, and determine strong zero-divisors of matrix rings over commutative rings with identity.

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49

Gao, Fuchang. "Non-zero boundaries of Leibniz half-spaces." Proceedings of the American Mathematical Society 133, no. 6 (2004): 1757–62. http://dx.doi.org/10.1090/s0002-9939-04-07732-9.

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50

Nixon, C. J., and J. E. Pringle. "Accretion discs with non-zero central torque." New Astronomy 85 (May 2021): 101493. http://dx.doi.org/10.1016/j.newast.2020.101493.

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