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1

Mohammed, Abdul Kadhim Al –. Sadi*. "MIXED SYMMETRY STATES IN SAMARIUM ISOTOPES WITH A=146-154 BY USING (IBM-2)." INTERNATIONAL JOURNAL OF ENGINEERING SCIENCES & RESEARCH TECHNOLOGY 6, no. 10 (2017): 413–21. https://doi.org/10.5281/zenodo.1036266.

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In this work, we used tthe (IBM-2) to study the mixed symmetry state property (MSS) foreven-even<sup>146-152</sup>Sm isotopes, this model gave a good agreementfor the excited energy levels for the g- band and acceptable for quasi (β and γ) bands, Also identified and emphase some states un certain experimentally, Furthermore it have been studied the mixed symmetry state (MSS) for the states (,,,,) Which received a quick response when changing the Majorana parameters for these isotopes.Well, it was calculated the electromagnetic transition B(E2), B(M1) and mixing ratios
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2

Gupta, Kumar S., and Amilcar de Queiroz. "Anomalies and renormalization of mixed states in quantum theories." Modern Physics Letters A 29, no. 13 (2014): 1450064. http://dx.doi.org/10.1142/s0217732314500643.

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In a Hamiltonian approach to anomalies, parity and time-reversal symmetries can be restored by introducing suitable impure (or mixed) states. However, the expectation values of observables such as the Hamiltonian diverges in such impure states. Here, we show that such divergent expectation values can be treated within a renormalization group (RG) framework, leading to a set of β-functions in the moduli space of the operators representing the observables. This leads to well-defined expectation values of the Hamiltonian in a phase where the impure state restores the P and T symmetry. We also sho
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3

Marczenko, M., D. Blaschke, K. Redlich, and C. Sasaki. "Toward a unified equation of state for multi-messenger astronomy." Astronomy & Astrophysics 643 (November 2020): A82. http://dx.doi.org/10.1051/0004-6361/202038211.

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Aims. We aim to present a first step in developing a benchmark equation-of-state (EoS) model for multi-messenger astronomy that unifies the thermodynamics of quark and hadronic degrees of freedom. Methods. A Lagrangian approach to the thermodynamic potential of quark-meson-nucleon matter was used. In this approach, dynamical chiral-symmetry breaking is described by the scalar mean-field dynamics coupled to quarks and nucleons and their chiral partners, whereby its restoration occurs in the hadronic phase by parity doubling, as well as in the quark phase. Quark confinement was achieved by an au
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4

LI, JIAN-FENG, HONG-TAO FENG, YU JIANG, WEI-MIN SUN, and HONG-SHI ZONG. "INFLUENCE OF A UNIFORM MAGNETIC FIELD ON DYNAMICAL CHIRAL SYMMETRY BREAKING IN QED3." Modern Physics Letters A 27, no. 09 (2012): 1250026. http://dx.doi.org/10.1142/s0217732312500265.

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We study dynamical chiral symmetry breaking (DCSB) in an effective QED3 theory of d-wave high temperature cuprate superconductors under a uniform magnetic field. At zero temperature, the external magnetic field induces a mixed state by generating vortices in the condensate of charged holons. The growing magnetic field suppresses the superfluid density and thus reduces the gauge field mass which is opened via the Anderson–Higgs mechanism. By numerically solving the Dyson–Schwinger gap equation, we show that the massless fermions acquires a dynamical gap through DCSB mechanism when the magnetic
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5

Azad, A. K., S. G. Eriksson, Håkan Rundlöf, and J. Eriksen. "Synthesis and Crystal Structure of the Double Perovskite Ca2-xSrxMnWO6 (x = 0.0, 0.5, 1.0, 1.5, 2.0)." Materials Science Forum 443-444 (January 2004): 375–78. http://dx.doi.org/10.4028/www.scientific.net/msf.443-444.375.

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The double perovskites Ca2-xSrxMnWO6(x = 0.0, 0.5, 1.0, 1.5, 2.0) have been prepared as pure phases by a conventional solid-state reaction process. Stoichiometric amounts of CaCO3,SrCO3, MnO and WO3were mixed, ground and calcined in a nitrogen atmosphere. X-ray and neutron powder diffraction (NPD), together with magnetisation measurements were carried out in order to characterise the materials. The NPD and magnetisation measurements, performed at different temperatures, were made in order to correlate the materials structural and magnetic properties. Susceptibility- Temperature (ϰ-T) curves we
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6

Lisińska-Czekaj, Agata, Henryk Bernard, Katarzyna Osinska, Jolanta Dzik, and Dionizy Czekaj. "Fabrication of La-Doped Bi4Ti3O12 Ceramics." Materials Science Forum 730-732 (November 2012): 105–10. http://dx.doi.org/10.4028/www.scientific.net/msf.730-732.105.

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La-modified Bi4Ti3O12 is a typical ferroelectric, piezoelectric and electro-optic material, having relatively low coercive field, low dielectric constant, high Curie temperature and high breakdown strength. Goal of the present research was to apply mixed oxide method for fabrication of BiTLax ceramics, study its chemical composition, crystalline structure and microstructure. The compound BiTLax for x=0, 0.25, 0.5, 0.75 ceramic powders were prepared from mixture of oxides by a solid state reaction at T=1000°C for t=3h. Ceramic powders of BiTLax were next press and the compacts were sintered by
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7

Carpenter, M. A., M. T. Zanni, D. J. Levandier, D. F. Varley, and J. M. Farrar. "Proton transfer dynamics on highly attractive potential energy surfaces: Induced repulsive energy release in O− + HF at high collision energies." Canadian Journal of Chemistry 72, no. 3 (1994): 828–35. http://dx.doi.org/10.1139/v94-110.

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We present the angular and kinetic energy distributions for the products of the proton transfer reaction O− + HF → OH + F− at center-of-mass collision energies of 45.0 and 55.8 kJ mol−l (0.47 and 0.58 eV, respectively). At both collision energies, the product angular distributions show forward–backward symmetry, characteristic of the decay of a transient complex living at least several rotational periods. The product kinetic energy distributions show structure that is clearly attributable to the formation of OH in v′ = 0,1, and 2. The kinetic energy distribution for a single vibrational state
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8

Syahbana, Muhammad Fauzan, Ahmad Jafar Arifi, and Terry Mart. "Distribution amplitude and decay constant of 1S and 2S state light mesons in the light-front quark model." ITM Web of Conferences 61 (2024): 01014. http://dx.doi.org/10.1051/itmconf/20246101014.

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Studying meson structures is essential for gaining insights into the nonperturbative nature of Quantum Chromodynamics (QCD). This study will focus on calculating the decay constant and distribution amplitudes (DAs) of unflavored light mesons (π and ρ) in the 1S and 2S states using the Light Front Quark Model. This study utilizes the QCD-motivated Hamiltonian, taking into account both contact and smeared spin-spin interactions. The two lowest harmonic oscillator bases are employed in this work to achieve improved results for the 2S states. The study found the optimal mixing parameter in basis e
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9

Bhaduri, Susmita, and Anirban Bhaduri. "Searching for Supersymmetry at LHC Using the Complex-Network-Based Method of the Three-Dimensional Visibility-Graph." Physics 2, no. 3 (2020): 436–54. http://dx.doi.org/10.3390/physics2030025.

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For the last several decades, there has been tremendous interest in search for Supersymmetry (SUSY) in the area of high energy physics. At Large Hadron Collider (LHC), there have been continuous searches for SUSY for prompt and non-prompt, for particle R-parity conserving and R-parity violating generation and decays. The limits obtained from these experiments and analyses for detection of the signatures of supersymmetric particles (LSP), revealed greater possibilities of such experiments in the collider. However, these signatures are usually derived under the assumption of bit optimistic condi
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10

Garau, Alessandra, Giacomo Picci, Massimiliano Arca, et al. "Can Serendipity Still Hold Any Surprises in the Coordination Chemistry of Mixed-Donor Macrocyclic ligands? The Case Study of Pyridine-Containing 12-Membered Macrocycles and Platinum Group Metal ions PdII, PtII, and RhIII." Molecules 26, no. 5 (2021): 1286. http://dx.doi.org/10.3390/molecules26051286.

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This study investigates the coordination chemistry of the tetradentate pyridine-containing 12-membered macrocycles L1-L3 towards Platinum Group metal ions PdII, PtII, and RhIII. The reactions between the chloride salts of these metal ions and the three ligands in MeCN/H2O or MeOH/H2O (1:1 v/v) are shown, and the isolated solid compounds are characterized, where possible, by mass spectroscopy and 1H- and 13C-NMR spectroscopic measurements. Structural characterization of the 1:1 metal-to-ligand complexes [Pd(L1)Cl]2[Pd2Cl6], [Pt(L1)Cl](BF4), [Rh(L1)Cl2](PF6), and [Rh(L3)Cl2](BF4)·MeCN shows the
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11

Börner, Martin, Laura Blömer, Marcus Kischel, et al. "Deposition of exchange-coupled dinickel complexes on gold substrates utilizing ambidentate mercapto-carboxylato ligands." Beilstein Journal of Nanotechnology 8 (July 5, 2017): 1375–87. http://dx.doi.org/10.3762/bjnano.8.139.

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The chemisorption of magnetically bistable transition metal complexes on planar surfaces has recently attracted increased scientific interest due to its potential application in various fields, including molecular spintronics. In this work, the synthesis of mixed-ligand complexes of the type [NiII 2L(L’)](ClO4), where L represents a 24-membered macrocyclic hexaazadithiophenolate ligand and L’ is a ω-mercapto-carboxylato ligand (L’ = HS(CH2)5CO2 − (6), HS(CH2)10CO2 − (7), or HS(C6H4)2CO2 − (8)), and their ability to adsorb on gold surfaces is reported. Besides elemental analysis, IR spectroscop
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12

WIEDENHOVER, I. "A mixed symmetry 2+ state in 132Ce." Progress in Particle and Nuclear Physics 38 (1997): 245–46. http://dx.doi.org/10.1016/s0146-6410(97)00032-x.

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13

Eid, S. A. A., W. D. Hamilton, and J. P. Elliott. "A shared mixed-symmetry state in 56Fe." Physics Letters B 166, no. 3 (1986): 267–68. http://dx.doi.org/10.1016/0370-2693(86)90795-1.

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14

Magdau, Ioan, Ross Howie, Graeme Ackland, and Eugene Gregoryanz. "Dynamical effects in solid hydrogen and hydrogen-deuterium mixtures at elevated pressures." Acta Crystallographica Section A Foundations and Advances 70, a1 (2014): C899. http://dx.doi.org/10.1107/s2053273314091001.

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We employed molecular dynamics simulations together with some novel theoretical techniques to calculate finite temperature Raman spectra in both hydrogen (H) and hydrogen-deuterium (HD) mixtures. By conditioning the simulations with the experimental data, we have discovered the true nature of Phase IV in solid hydrogen. X-ray and neutron diffraction measurements are virtually impossible in current state of the art experiments. The experimental investigation, thus, relies mainly on spectroscopic methods which provide minimal data about crystallography. Extensive work done so far [1] has led to
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15

Lee, Jong Yeon, Yi-Zhuang You, and Cenke Xu. "Symmetry protected topological phases under decoherence." Quantum 9 (January 23, 2025): 1607. https://doi.org/10.22331/q-2025-01-23-1607.

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We investigate mixed states exhibiting nontrivial topological features, focusing on symmetry-protected topological (SPT) phases under various types of decoherence. Our findings demonstrate that these systems can retain topological information from the SPT ground state despite decoherence. In the &amp;apos;&amp;apos;doubled Hilbert space,&amp;apos;&amp;apos; we define symmetry-protected topological ensembles (SPT ensembles) and examine boundary anomalies in this space. We generalize the concept of the strange correlator, initially used to diagnose SPT ground states, to identify anomalies in mix
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16

Fazzini, T. F., A. Giannatiempo, A. Nannini, A. Perego, and D. Cutoiu. "Search for the lowest 2+ mixed-symmetry state in102Ru." Zeitschrift f�r Physik A Hadrons and Nuclei 346, no. 1 (1993): 21–24. http://dx.doi.org/10.1007/bf01290777.

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17

WANG, Z. D., Q. LI, and Q. H. WANG. "GINZBURG-LANDAU THEORY OF MIXED WAVE SUPERCONDUCTORS." International Journal of Modern Physics B 13, no. 29n31 (1999): 3569–72. http://dx.doi.org/10.1142/s0217979299003441.

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We address vortex state and dynamics of mixed wave superconductors in the framework of Ginzburg-Landau theory. We find that the s- and d-wave components of a single vortex in the d+is-state exhibit two-fold symmetry and the intrinsic Hall effect displays a different angle dependence from that of d-wave state. For dx2-y2+idxy-wave superconductors, a Ginzburg-Landau theory is developed from a microscopic theory with a strong coupling term being included. In the absence of a magnetic field, the theory predicts a pure dx2-y2 state at T&gt;T* and a second order phase transition at T* to a time-reve
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18

Scheck, M., E. T. Gregor, M. Thürauf, et al. "Candidates for low-lying octupole isovector (mixed-symmetry) excitations." EPJ Web of Conferences 329 (2025): 01001. https://doi.org/10.1051/epjconf/202532901001.

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The spectroscopic properties of low-lying octupole states, previously proposed to be candidates for isovector (mixed-symmetry) states, were investigated in 95Mo(nth, γ) and 143Nd(nth, γ) thermal neutron capture reactions. The experiments used eight Clover detectors that made up the central ring of the EXILL setup and the high thermal neutron flux of the research reactor at ILL. These measurements allowed a determination of branching ratios and multipole mixing ratios for the transitions of interest connecting the isovector candidate and the lowest-lying Jπ = 3−1 state, the octupole phonon. Fur
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19

Wiedenhöver, I., A. Gelberg, T. Otsuka, et al. "2+mixed symmetry state in the O(6)-like nucleus128Xe." Physical Review C 56, no. 5 (1997): R2354—R2357. http://dx.doi.org/10.1103/physrevc.56.r2354.

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20

Luk'yanchuk, I., and M. Zhitomirsky. "Symmetry of the mixed state of superconductors with anisotropic pairing." Physica C: Superconductivity 206, no. 3-4 (1993): 373–86. http://dx.doi.org/10.1016/0921-4534(93)90537-z.

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21

Addicoat, Magdalene A., Mark A. Buntine, and Gregory F. Metha. "DFT Calculations on Group 5 Mixed Metal Tetramers: TaxNbyVz (x + y + z = 4)." Australian Journal of Chemistry 57, no. 12 (2004): 1197. http://dx.doi.org/10.1071/ch04122.

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We report Density Functional Theory (DFT) calculations on mixed-metal tetramers comprised of the Group 5 (Vb) elements V, Nb, and Ta. Our results show that the lowest energy structures for Nb4 and Ta4 are regular tetrahedra with Td symmetry and singlet multiplicity whereas V4 is a triplet state with C2v symmetry. The monosubstituted isomers, A3B, all have C3v symmetry but several higher energy Cs structures have been found that are approximately 100 kJ mol−1 higher in energy. The disubstituted isomers all posses arachno-butterfly structures; the A2B2 types with C2v symmetry and the A2BC types
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22

Wasielewski, Michael R., Chenjian Lin, Taeyeon Kim, Jonathan D. Schultz, and Ryan M. Young. "(Invited) Ultrafast Symmetry-Breaking Charge Separation in Organic Semiconductors." ECS Meeting Abstracts MA2022-02, no. 48 (2022): 1839. http://dx.doi.org/10.1149/ma2022-02481839mtgabs.

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Understanding the photophysics and photochemistry of molecular π-stacked chromophores is important for utilizing them as functional photonic materials. However, these investigations have been mostly limited to covalent molecular dimers, which can only approximate the electronic and vibronic interactions present in higher oligomers typical of functional organic materials. In this work, we show that a comparison of the excited-state dynamics of a covalent slip-stacked perylenediimide (PDI) dimer(1)and trimer (2) provides fundamental insights into electronic state mixing and symmetry-breaking cha
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23

Fil, V. D., D. V. Fil, G. A. Zvyagina, I. V. Bilych, and K. R. Zhekov. "Piezomagnetism in a mixed state in FeSe-based superconductors." Low Temperature Physics 49, no. 5 (2023): 614. http://dx.doi.org/10.1063/10.0017823.

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The acoustoelectric transformation (AET) in the mixed state of FeSe-based superconducting chalcogenides was studied. Dependence of the AET signal on the magnetic field obtained at the initial stages of flux penetration shows a behavior that can be explained only if the piezomagnetism is included in the consideration. This argues that these crystals belong to the class of compounds with broken time-reversal symmetry and are in a state of hidden magnetic order.
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Yamagata, Hirokazu, and Hidetoshi Fukuyama. "Infrared Optical Conductivity in Superconducting State with Mixed Symmetry Gap Function." Journal of the Physical Society of Japan 65, no. 7 (1996): 2204–11. http://dx.doi.org/10.1143/jpsj.65.2204.

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25

Journal, Baghdad Science. "The Prediction of the Electromagnetic Properties and the ?(E2/M1) of 110-116Cd-Isotopes in IBM Model." Baghdad Science Journal 8, no. 3 (2011): 772–80. http://dx.doi.org/10.21123/bsj.8.3.772-780.

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The Nuclear structure of 110-116Cd isotopes was studied theoretically in the framework of the interacting boson model of IBM-l and IBM-2. The properties of the lowest mixed symmetry states such as the 1+, 2+ and 3+ levels produced by the IBM-2 model in the vibrational-limit U(5) of Cd - isotopes are studied in details. This analysis shows that the character of mixed symmetry of 2+ is shared between and states in 110-114Cd – isotopes, the large shar goes to s, while in isotope, the state is declared as a mixed symmetry state without sharing. This identification is confirmed by the percentage of
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Ahmad, Saddon Taha, and Diary Omar Kakil. "The Prediction of the Electromagnetic Properties and the ?(E2/M1) of 110-116Cd-Isotopes in IBM Model." Baghdad Science Journal 8, no. 3 (2011): 772–80. http://dx.doi.org/10.21123/bsj.2011.8.3.772-780.

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The Nuclear structure of 110-116Cd isotopes was studied theoretically in the framework of the interacting boson model of IBM-l and IBM-2. The properties of the lowest mixed symmetry states such as the 1+, 2+ and 3+ levels produced by the IBM-2 model in the vibrational-limit U(5) of Cd - isotopes are studied in details. This analysis shows that the character of mixed symmetry of 2+ is shared between and states in 110-114Cd – isotopes, the large shar goes to s, while in isotope, the state is declared as a mixed symmetry state without sharing. This identification is confirmed by the percentage of
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27

Bu, Kejun, Jianqiao He, Dong Wang, Chong Zheng, and Fuqiang Huang. "Crystal structure of the mixed-metal trisulfide BaCu1/3Ta2/3S3." Acta Crystallographica Section E Crystallographic Communications 73, no. 5 (2017): 713–15. http://dx.doi.org/10.1107/s2056989017005266.

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The mixed-metal title compound, BaCu1/3Ta2/3S3[barium copper(II) tantalum(V) trisulfide], was prepared through solid-state reactions. The crystal structure adopts the BaTaS3structure type and consists of face-sharing [MS6] (M= Ta,Cu) octahedra (point-group symmetry -3m.) that are condensed into infinite chains along [001]. Adjacent chains are linked through the barium cations (site symmetry -6m2), which exhibit a coordination number of twelve. TheMsite is occupied by 2/3 of TaVand 1/3 of CuII, whereby the averageM—S distances are slightly longer than those of ordered BaTaS3. The classical char
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28

Hu, Yongbing, Chenchong Bi, and Yong Chen. "Kernel Adaptive Filtering Algorithm Based on Hyperbolic Tangent Mixed Error Function." Symmetry 16, no. 12 (2024): 1624. https://doi.org/10.3390/sym16121624.

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This paper proposes an adaptive filtering algorithm based on the symmetry Kernel Hyperbolic Tangent Mixed Error Criterion (KHTMC), aimed at addressing the identification of nonlinear systems under non-Gaussian noise environments. The algorithm optimizes signal processing by constructing a mixed cost function that combines the symmetry logarithmic square error and the hyperbolic tangent function and integrates it with the kernel adaptive filtering method. Simulation results show that, compared to existing kernel adaptive filtering algorithms, the KHTMC algorithm exhibits significant advantages
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Muto, Takumi, Toshiki Maruyama, and Toshitaka Tatsumi. "Chiral Symmetry in Dense Matter with Meson Condensation." Symmetry 17, no. 2 (2025): 270. https://doi.org/10.3390/sym17020270.

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Kaon condensation in hyperon-mixed matter [(Y+K) phase], which may be realized in neutron stars, is discussed on the basis of chiral symmetry. With the use of the effective chiral Lagrangian for kaon–baryon and kaon–kaon interactions; coupled with the relativistic mean field theory and universal three-baryon repulsive interaction, we clarify the effects of the s-wave kaon–baryon scalar interaction simulated by the kaon–baryon sigma terms and vector interaction (Tomozawa–Weinberg term) on kaon properties in hyperon-mixed matter, the onset density of kaon condensation, and the equation of state
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30

Eltschka, Christopher, and Jens Siewert. "Optimal class-specific witnesses for three-qubit entanglement from Greenberger-Horne-Zeilinger symmetry." Quantum Information and Computation 13, no. 3&4 (2013): 210–20. http://dx.doi.org/10.26421/qic13.3-4-3.

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Recently, a new type of symmetry for three-qubit quantum states was introduced, the so-called Greenberger-Horne-Zeilinger (GHZ) symmetry. It includes the operations which leave the three-qubit standard GHZ state unchanged. This symmetry is powerful as it yields families of mixed states that are, on the one hand, complex enough from the physics point of view and, on the other hand, simple enough mathematically so that their properties can be characterized analytically. We show that by using the properties of GHZ-symmetric states it is straightforward to derive optimal witnesses for detecting cl
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BELOVA, POLINA, IVAN ZAKHARCHUK, KONSTANTIN BORISOVICH TRAITO, and ERKKI LÄHDERANTA. "IMPACT OF THE ORDER PARAMETER SYMMETRIES ON THE VORTEX CORE STRUCTURE IN IRON-BASED SUPERCONDUCTORS." Modern Physics Letters B 26, no. 21 (2012): 1230013. http://dx.doi.org/10.1142/s021798491230013x.

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Effects of the order parameter symmetries on the cutoff parameter ξh (determining the magnetic field distribution) in the mixed state are investigated in the framework of quasiclassical Eilenberger theory for isotropic s±, s++ and anisotropic dx2-y2-wave superconducting pairings. These symmetries are proposed for the pairing state of the Fe -pnictides. In s± pairing symmetry, the gap function has opposite sign at the electron and hole pockets of the Fermi surface, it is connected with interband antiferromagnetic spin fluctuations. In s++ pairing symmetry, the gap function has the same sign at
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32

Coser, Andrea, and David Pérez-García. "Classification of phases for mixed states via fast dissipative evolution." Quantum 3 (August 12, 2019): 174. http://dx.doi.org/10.22331/q-2019-08-12-174.

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We propose the following definition of topological quantum phases valid for mixed states: two states are in the same phase if there exists a time independent, fast and local Lindbladian evolution driving one state into the other. The underlying idea, motivated by \cite{Konig2014}, is that it takes time to create new topological correlations, even with the use of dissipation.We show that it is a good definition in the following sense: (1) It divides the set of states into equivalent classes and it establishes a partial order between those according to their level of ``topological complexity''.
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Mehlich, Christine, and Christoph van Wüllen. "Hyperfine tensors for a model system for the oxygen evolving complex of photosystem II: calculation of the anisotropy shift that occurs beyond the strong exchange limit." Physical Chemistry Chemical Physics 21, no. 41 (2019): 22902–9. http://dx.doi.org/10.1039/c9cp03629f.

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Broken-symmetry density functional calculations have been used to calculate effective <sup>55</sup>Mn hyperfine (A) tensors for a mixed-valence tetranuclear manganese complex, a model system for the S<sub>2</sub> state of the oxygen-evolving complex of photosystem II.
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Daiji, Yongzhi, Shuibo Huang, and Qiaoyu Tian. "Symmetry and Monotonicity of Solutions to Mixed Local and Nonlocal Weighted Elliptic Equations." Axioms 14, no. 2 (2025): 139. https://doi.org/10.3390/axioms14020139.

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This paper focuses on the symmetry and monotonicity of non-negative solutions to a mixed local and nonlocal weighted elliptic problem. This problem generalizes the ground-state representation of elliptic equations with the Hardy potential. The novelty of this research lies in developing the moving planes method for mixed local and nonlocal equations with a weighted function, thus clarifying the influence of the weighted function on the solution properties.
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35

Sato, Yohei, and Zhi-Qiang Wang. "Least Energy Solutions for Nonlinear Schrödinger Systems with Mixed Attractive and Repulsive Couplings." Advanced Nonlinear Studies 15, no. 1 (2015): 1–22. http://dx.doi.org/10.1515/ans-2015-0101.

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AbstractIn this paper we study the ground state solutions for a nonlinear elliptic system of three equations which comes from models in Bose-Einstein condensates. Comparing with existing works in the literature which have been on purely attractive or purely repulsive cases, our investigation focuses on the effect of mixed interaction of attractive and repulsive couplings. We establish the existence of least energy positive solutions and study asymptotic profile of the ground state solutions, giving indication of co-existence of synchronization and segregation. In particular we show symmetry br
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36

Najy Hady, Heiyam, and Ruqaya Talib Kadhim. "Mixed symmetry states in 96Mo and 98Ru isotones in the framework of interacting boson model." 3C Empresa. Investigación y pensamiento crítico 12, no. 01 (2023): 243–55. http://dx.doi.org/10.17993/3cemp.2023.120151.243-255.

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The software package IBM code for interacting boson model-1 and Neutron Proton Boson NPBOS code for interacting boson model-2 have been used to calculate energy levels for, for by estimating a set of parameters which are used to predict the behavior of even-even isotones within the current scope of work there is clear competition between the two parameters (ε and a2) in isotones, as an inverse relationship. This means that vibrational qualities are continuous mixed with the rotational properties. In interacting boson model-2 parameters(ε, κ, χπ and χν) have been shown similarity with interacti
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37

Curtis, Macauley, Martin Gradhand, and James F. Annett. "Simple Model for Tc and Pairing Symmetry Changes in Sr2RuO4 Under (100) Uniaxial Strain." Condensed Matter 9, no. 4 (2024): 44. http://dx.doi.org/10.3390/condmat9040044.

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Uniaxial strain in the (100) direction has the effect of increasing the superconducting Tc in Sr2RuO4 from 1.5 K to over 3 K. The enhanced Tc corresponds to a Lifshitz transition in the Fermi surface topology of this unconventional superconductor. We model this using a simple two-dimensional one-band model for the γ sheet of the Fermi surface. This reproduces the experimental Tc results well if we assume a dx2−y2 singlet pairing state. On the other hand, the triplet state px+ipy does not show any distinct peaks in Tc associated with the Lifshitz transition. A mixed symmetry state pairing of th
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38

Stamatatos, Theocharis C., Khalil A. Abboud, Wolfgang Wernsdorfer, and George Christou. "High-Nuclearity, High-Symmetry, High-Spin Molecules: A Mixed-Valence Mn10 Cage Possessing RareT symmetry and anS=22 Ground State." Angewandte Chemie 118, no. 25 (2006): 4240–43. http://dx.doi.org/10.1002/ange.200600691.

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39

Stamatatos, Theocharis C., Khalil A. Abboud, Wolfgang Wernsdorfer, and George Christou. "High-Nuclearity, High-Symmetry, High-Spin Molecules: A Mixed-Valence Mn10 Cage Possessing RareT symmetry and anS=22 Ground State." Angewandte Chemie International Edition 45, no. 25 (2006): 4134–37. http://dx.doi.org/10.1002/anie.200600691.

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40

Jennings, R. L., and N. O. Weiss. "Symmetry Breaking in the Solar Dynamo: Nonlinear Solutions." Symposium - International Astronomical Union 138 (1990): 355–58. http://dx.doi.org/10.1017/s0074180900044338.

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We examine an idealized αω-dynamo model in which the magnetic fields depend only on latitude and time. The solutions that bifurcate from the field-free state are either symmetric or antisymmetric about the equator (quadrupolar or dipolar respectively). Nonlinear steady and periodic solutions, whether stable or unstable, can be followed numerically as the dynamo number is varied, revealing a rich bifurcation structure with mixed-mode solutions (lacking symmetry about the equator) appearing at secondary bifurcations. These results show how stable asymmetric fields can occur in the sun and illust
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41

Fransen, C., N. Pietralla, P. von Brentano, et al. "First observation of a mixed-symmetry two-Q-phonon 22,ms+ state in 94Mo." Physics Letters B 508, no. 3-4 (2001): 219–24. http://dx.doi.org/10.1016/s0370-2693(01)00345-8.

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42

Rutkevich, S. B. "On the absence of long-range order in a type II superconductor in the mixed state." Soviet Journal of Low Temperature Physics 16, no. 3 (1990): 157–59. https://doi.org/10.1063/10.0032504.

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It is shown that the violation of the long-range superconducting order in Abrikosov’s vortex lattices predicted by Maki and Takayama on the basis of an approximate approach that was valid only in the vicinity of Hc2(T), is indeed an exact result governed only by the symmetry properties of a superconductor in a magnetic field.
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43

BHATTACHARYYA, P. "SPIN FLUCTUATION INDUCED PAIRING FOR HIGH Tc COMPOUNDS." Modern Physics Letters B 04, no. 18 (1990): 1177–84. http://dx.doi.org/10.1142/s0217984990001483.

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We show that measurements of the upper critical field can, within the context of the pairing hypothesis, distinguish between spin fluctuation dominated pairing and those that do not involve spin. Comparison with experiments supports the hypothesis that the dominant pairing interaction in high Tc compounds is spin fluctuation induced. We also show the existence of a new mode in the mixed state, the mid-gap state, which is an immediate consequence of gauge symmetry.
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44

Liu, Xue-Ke, and Xiao-Yong Wen. "Continuous Limit, Rational Solutions, and Asymptotic State Analysis for the Generalized Toda Lattice Equation Associated with 3 × 3 Lax Pair." Symmetry 14, no. 5 (2022): 920. http://dx.doi.org/10.3390/sym14050920.

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Discrete integrable nonlinear differential difference equations (NDDEs) have various mathematical structures and properties, such as Lax pair, infinitely many conservation laws, Hamiltonian structure, and different kinds of symmetries, including Lie point symmetry, generalized Lie bäcklund symmetry, and master symmetry. Symmetry is one of the very effective methods used to study the exact solutions and integrability of NDDEs. The Toda lattice equation is a famous example of NDDEs, which may be used to simulate the motions of particles in lattices. In this paper, we investigated the generalized
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45

Sundermann, Martin, Maurits W. Haverkort, Stefano Agrestini, et al. "Direct bulk-sensitive probe of 5fsymmetry in URu2Si2." Proceedings of the National Academy of Sciences 113, no. 49 (2016): 13989–94. http://dx.doi.org/10.1073/pnas.1612791113.

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The second-order phase transition into a hidden order phase in URu2Si2goes along with an order parameter that is still a mystery, despite 30 years of research. However, it is understood that the symmetry of the order parameter must be related to the symmetry of the low-lying local electronicf-states. Here, we present results of a spectroscopic technique, namely core-level nonresonant inelastic X-ray scattering (NIXS). This method allows for the measurement of local high-multipole excitations and is bulk-sensitive. The observed anisotropy of the scattering function unambiguously shows that the
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46

YU, HONG-YI, FA-DI SUN, and AN-CHUN JI. "GOSSAMER SUPERFLUID AND ANTIFERROMAGNETIC STATE OF COLD ATOMS IN OPTICAL LATTICES." Modern Physics Letters B 24, no. 23 (2010): 2377–86. http://dx.doi.org/10.1142/s0217984910024833.

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We propose a scheme to simulate the t–J–U model and investigate the quantum phase transitions using cold atoms confined in a two-dimensional optical lattice. By adjusting the parameters of external laser fields, we find a phase transition from antiferromagnetic phase to Gossamer superfluid. The Gossamer superfluid has a d-wave or mixed d- and s-wave symmetry, depending on the hopping parameters which can be adjusted by tuning the laser field. Experimental protocol to observe these new phenomena for future experiments has also been briefly discussed.
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47

Arraut, Ivan. "A Possible Solution to the Black Hole Information Paradox." AppliedMath 5, no. 1 (2025): 4. https://doi.org/10.3390/appliedmath5010004.

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The information paradox suggests that the black hole loses information when it emits radiation. In this way, the spectrum of radiation corresponds to a mixed (non-pure) quantum state even if the internal state generating the black hole is expected to be pure in essence. In this paper we propose an argument solving this paradox by developing an understanding of the process by which spontaneous symmetry breaks when a black hole selects one of the many possible ground states and emits radiation as a consequence of it. Here, the particle operator number is the order parameter. This mechanism expla
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48

Nakashima, Satoru, Takashi Oda, and Tsutomu Okuda. "Effects of Cation Symmetry and its Packing on the Mixed-Valence State of Binuclear Ferrocenes." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 342, no. 1 (2000): 267–72. http://dx.doi.org/10.1080/10587250008038276.

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49

Luk'yanchuk, I., and M. Zhitomirsky. "Superconducting mixed state symmetry for an anisotropic pairing near Hc2 and phase transitions in UPt3." Physica C: Superconductivity 185-189 (December 1991): 2629–30. http://dx.doi.org/10.1016/0921-4534(91)91437-9.

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50

Kovalchuk, Valery I. "Solution of Faddeev integral equations in configuration space using the hyperspherical harmonics expansion method." International Journal of Modern Physics E 23, no. 11 (2014): 1450069. http://dx.doi.org/10.1142/s0218301314500694.

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In this paper, a method has been developed to solve three-particle Faddeev equations in the configuration space making use of a series expansion in hyperspherical harmonics. The following parameters of the bound state of triton and helium-3 nuclei have been calculated: the binding energies, the weights of symmetric and mixed-symmetry components of the wave function, the magnetic moments, and the charge radii.
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