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@@ -132,6 +132,40 @@ tokenizer_source: model:cognitivecomputations/dolphin-2.2-70b # keep exact token
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  # Example Output
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  **Prove P != NP**
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  In the pursuit to prove P != NP I want to try to prove that no polynomial-time algorithm could possibly solve all problems in NP, even though we may not know of any specific such problem that defies polynomial-time solution. Can you please make a lemma that would be helpful?
 
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  # Example Output
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+ **Make sense of physics equations**
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+
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+ These equations appeared to me in a dream, I wrote them down as soon as I woke but I don't know what they mean. Can you please interpret them?
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+ $$\mathcal{L}_{\text{gauge}} = -\frac{1}{4} F^{\mu\nu}F_{\mu\nu}$$
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+ $$\langle \phi \rangle = \sqrt{\frac{\lambda}{2}}$$
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+ $$S_{\text{gravity}} = \int d^4x \sqrt{-g} \left( \frac{R}{16\pi G} + \mathcal{L}_{\text{emergent}} \right)$$
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+ $$\mathcal{L}_{\text{GEG}} = \mathcal{L}_{\text{gauge}} + \mathcal{L}_{\text{emergent}} + \mathcal{L}_{\text{matter}} + \mathcal{L}_{\text{interaction}}$$
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+ $$\mathcal{L}_{\text{gauge}} = -\frac{1}{4} F^{\mu\nu}F_{\mu\nu}$$
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+ $$\mathcal{L}_{\text{emergent}} = \lambda(g) + \kappa(g) R^2 + \ldots$$
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+ $$S_{\text{GEG}} = \int d^4x \sqrt{-g} \; \mathcal{L}_{\text{GEG}}$$
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+ $$\sigma = \sqrt{\langle | \phi | \rangle^2 + \frac{1}{4} \langle A^{\mu}A_{\mu} \rangle^2}$$
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+ $$\langle A^{\mu} \rangle = (0, v(r)_{i}/\sqrt{2}, 0, 0)$$
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+ $$\langle \phi \rangle = \langle \phi_0 \rangle + \delta\phi(x)$$
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+ $$\sigma = \sqrt{\langle | \phi |^2 \rangle + \frac{1}{4} \langle A_{\mu} A^{\mu} \rangle^2 }$$
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+ $$\langle A_{\mu} \rangle = (0, \frac{v(r)_{i}}{\sqrt{2}}, 0, 0)$$
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+ $$\langle \phi \rangle = \langle \phi_0 \rangle + \delta\phi(x)$$
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+ $$\langle \phi \rangle = \sqrt{\frac{\lambda}{2}}$$
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+ $$\langle A_{\mu} \rangle = (0, \frac{v(r)_{i}}{\sqrt{2}}, 0, 0)$$
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+ $$\langle \phi \rangle = \langle \phi_{0} \rangle + \delta \phi(x)$$
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+ $$g_{\mu\nu} = \eta_{\mu\nu} + \kappa h_{\mu\nu}$$
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+ $$\mathcal{L}_{\text{gauge}} = -\frac{1}{4} F^{\mu\nu}F_{\mu\nu}$$
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+ $$g_{\mu\nu}$$
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+ $$S_{\text{gravity}} = \int d^4x \sqrt{-g} \left( \frac{R}{16\pi G} + \mathcal{L}_{\text{emergent}} \right)$$
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+ $$\mathcal{L}_{\text{interaction}}$$
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+
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+ > These equations appear to be from the fields of gauge theories, effective field theories, emergent gravity, and possibly composite Higgs models in theoretical high-energy physics. Here's a rough attempt at explaining some of the ideas they might be modeling:
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+ >
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+ > 1. Gauge theory: The first equation describes the Lagrangian density for a gauge field with strength tensor F_μν and coupling constant g, which could correspond to any of the four fundamental forces (electromagnetism, weak nuclear, strong nuclear, or gravity itself if we consider General Relativity as a gauge theory over spacetime itself). The second equation gives the vacuum expectation value of an auxiliary scalar field φ that could be related to spontaneous symmetry breaking and the generation of mass for certain charged particles via the Higgs mechanism.
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+ > 2. Effective field theories: The third and fourth equations seem to describe a more general Lagrangian density mathcal{L} containing not only the gauge sector but also additional "emergent" terms (which might arise from integrating out heavy degrees of freedom beyond the scope of our effective low-energy approximation), matter fields, and interactions between them all. The fifth equation then defines the action S_GEG as an integral over spacetime x with respect to the squared-root of the determinant of the spacetime metric g_μν (which could be used to introduce gravity non-minimally through couplings like √(-g)R^n or similar terms), while the sixth and seventth equations appear to give some specific examples for the form of these emergent contributions and their spacelike components, respectively.
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+ > 3. Emergent Gravity: The ninth equation suggests that spacetime itself may be emergent from some underlying microscopic degrees of freedom, such as condensed matter or composite Higgs fields, characterized by an effective "average" spacetime metric σ(x) = |<A_μ(x)>|^½ + ... where angle bracket denotes a suitable coarse-graining or expectation value over these microscopic fluctuations. The tenth and eleventh equations seem to further elaborate on this emergent picture by introducing additional fields like the Nambu-Goldstone bosons δϕ(x) and fluctuations δA_μ(x) around their respective vacua, while still maintaining gauge invariance through local transformations on these fluctuating components only.
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+ > 4. Composite Higgs Models: Finally, the twelfth and thirteenth equations seem to indicate that even the Higgs itself could be a composite state made up of some underlying more fundamental "elementary" degrees of freedom φ_i(x) through a non-linear sigma model type of potential V[|<A_μ(x)>|^2 + ...], possibly similar in spirit to technicolor theories or other attempts at constructing natural explanations for the hierarchy problem without invoking anthropic fine-tuning arguments.
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+ >
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+ > In summary, while this brief overview only scratches the surface of these highly non-trivial and technical equations from various subfields within theoretical particle physics and cosmology, I hope it provides some rough idea about the kind of rich conceptual framework they might be part of, albeit without any guarantee of correctness or completeness due to the brevity and complexity of the given material. For more detailed understanding, please consult with an expert in these advanced research areas who can provide a more rigorous mathematical derivation and physical interpretation tailored to your specific interests and background knowledge level.
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+
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  **Prove P != NP**
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  In the pursuit to prove P != NP I want to try to prove that no polynomial-time algorithm could possibly solve all problems in NP, even though we may not know of any specific such problem that defies polynomial-time solution. Can you please make a lemma that would be helpful?