tackle
发表于 2025-3-26 23:23:20
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Charlatan
发表于 2025-3-27 04:35:04
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腐蚀
发表于 2025-3-27 09:15:15
The Long Way to the Statistical Bootstrap Modelns to which they owe their existence. To simulate all . strong interactions we need all of them (including the not yet discovered ones), that is: we need the complete mass spectrum ρ(.). To simulate . forces we may use proper cluster volumes à la Van der Waals. In order to obtain the full mass spect
investigate
发表于 2025-3-27 11:53:17
Crystalline Quark-Hadron Phase in Neutron Starses is the Coulomb force, an intermediate-range order will be created by the competition between Coulomb and surface interface energy. Their sum is minimized when the coexistence phase assumes a Coulomb lattice of one phase immersed in the other. The geometry will vary continuously as the proportion
水土
发表于 2025-3-27 14:09:11
0258-1221 cs (QCD), and recognizing the im portant role of the complex QCD-vacuum structure. On the other side, we have developed new experimental tools in the form of n978-1-4613-5798-8978-1-4615-1945-4Series ISSN 0258-1221
MOAT
发表于 2025-3-27 18:47:19
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daredevil
发表于 2025-3-27 22:11:32
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忍耐
发表于 2025-3-28 04:57:53
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嬉耍
发表于 2025-3-28 06:55:26
Statistical Studies of Hadronsl Universe” on freshman physics, and the like. I am not currently active in studies of Hot Hadronic Matter. Therefore, this talk will be historical and reminiscent in nature. In brief, I’ll describe how I started with few-body issues, how the physics then led me to many-body and statistical studies,
抵消
发表于 2025-3-28 11:28:53
Hagedorn’s Temperature and the Dual Resonance Model: A 25 Year Old Love Affairy. Let me remind you that, by definition of (Dolen-Horn-Schmit) duality, the asymptotic behaviour of (the imaginary part of) any scattering amplitude should be correctly described . by Regge pole exchange in the t-channel or by resonance formation and decay in the s-channel.