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Prompt by IONFAST

1 --q 2 Stable Diffusion prompts

very few results

8 months ago

Renaissance-style oil painting with loose, textured brushstrokes of A young, fair-skinned woman stands in a field, her back to the viewer, looking at a small, aged-looking house in the distance. Her expression is contemplative, almost sad. She is wearing a long, full-skirted, antique-style white dress with a fitted bodice and intricate detailing. The dress appears to be made of a light, flowing fabric, and the skirt is adorned with intricate, textured embroidery. Simple, tight-fitting dark stockings and dark brown shoes complete her attire. The woman has long, dark brown hair, styled in a loose ponytail. Her body posture is straight and relaxed, suggesting a calm, yet thoughtful, demeanor. The field is a soft grayish-green color, consistent with a natural landscape on a cloudy day. The house in the distance is a light gray-tan color, with a simple, gabled roof and few distinguishing details, creating a sense of age and isolation. The overall color palette is muted and monochromatic, with soft grays, tans, and browns. The lighting suggests a soft, diffuse light source, with no harsh shadows and an overcast sky. The composition is centered on the woman, with the house in the background, creating a serene, almost melancholic mood. A vintage, slightly painterly style of photography with a soft focus creates a dreamy, introspective atmosphere. The photographic perspective is frontal, slightly elevated, allowing a focused view of the subject and environmental details. --ar 1:1.618 --q 2 --s 800

Morgue PRO
3 160

13 days ago

We consider the action $S_{\phi q}$ involving only $\phi_{\mu\nu}$ and quark fields $q(x)$ in general frames with Poincar\'e metric tensor $P_{\mu\nu}$: \be S_{\phi q} = \int (L_{\phi q} + L_{gf})d^4 x, \ee %%%%%%%%15%%%%22%%%%%24%%%22%%%19 \be L_{gf}=\frac{1}{2g^2}\e_{\a\b}\left[\p_\mu J^{\mu\a} - \frac{1}{2}\e^{\a\ld}\p_{\ld} J^\mu_\mu\right] \left[\p_\nu J^{\nu\b} - \frac{1}{2}\e^{\b\ld}\p_{\ld} J^\nu_\nu\right], \ee %%%%16%%%%%%%23%%%%%25%%%23%%%%20 where $L_{\phi q}$ is given in (7) with the $T(4)$ gauge curvature $C_{\mu\nu\a}$ given by (5). We have included a gauge-fixing term $L_{gf}$ specified by (20) involving ordinary partial derivative to break the $T(4)$ gauge symmetry so that the solution of gauge field equation is well-defined. The reason for including $L_{gf}$ is that field equations with gauge symmetry are known to be not well defined in general and that it is a nuisance to find explicit solutions of such field equations without having a gauge-fixing term. The quark fields play the source for producing a gravitational potential field $\phi_{\mu\nu}$. The $T(4)$ gravitational field equation for symmetric tensor field, $\phi_{\mu\nu}=\phi_{\nu\mu}$ can be derived from (19), \be H^{\mu\nu} + A^{\mu\nu}= \frac{g^2}{2} Sym \ \left[ \overline{q} i\G^\mu D^\nu q - i(D^\nu \overline{q}) \G^\mu q \right]\equiv g^2 T^{\mu\nu} , \ee %%%%%26%%%17%%%%%%%%%24%%%%%%26%%%24%21 $$ H^{\mu\nu} = Sym \left[D_\ld (J^{\ld}_\rho C^{\rho\mu\nu} - J^\ld_\a C^{\a\b}_{ \ \ \ \b}P^{\mu\nu} + C^{\mu\b}_{ \ \ \ \b} J^{\nu\ld}) \right. $$ %%%%%%%%%%%%%%%%%%%%%%%%20%%% \be \left. - C^{\mu\a\b}D^\nu J_{\a\b} + C^{\mu\b}_{ \ \ \ \b} D^\nu J^\a_\a - C^{\ld \b}_{ \ \ \ \b}D^\nu J^\mu _\ld\right], \ee %%%%%%%27 %%%%%%%%%%18%%%%%%%%%25%%%27%%%%25%%522 \be A^{\mu\nu} =Sym \left[ \p^\mu \left(\p^\ld J_\ld{^\nu} - \frac{1}{2} \p^\nu J \right) - \frac{\e^{\mu\nu}}{2} \left(\p^\a \p^\ld J_{\ld\a} - \frac{1}{2} \p^\a \p_\a J \right)\right], \ee %%%19%%%%%%%%%%26%%%%%%%%28%%%%%26%%%523 where $D_{\mu}q=\p_{\mu}q$ and $J= J^\ld_\ld$. The symbol `Sym' in Eqs. (21)-(23) denotes that $\mu$ and $\nu$ should be made symmetric.

620ba102fd7
0 17