#astronomyimpressionism

Literary Masterpieces - Life of Galileo by Bertolt Brecht

• Model: Nano Banana 2 (Pro)

• Size: 2240 X 1680 (3.76 MP)

• Used settings:

  • Prompt: Galileo standing in a dimly lit study filled with astronomical instruments, pointing toward a telescope aimed at the night sky. Through the window, stars shine vividly. Papers and sketches of planetary motion scatter across his desk. A sense of intellectual rebellion and discovery fills the air. Dramatic chiaroscuro lighting. Style by Caravaggio × Rembrandt × Zdzisław Beksiński (subtle influence), include a sterilized unicorn head logo and the text “AI by Unicorngraphics” as watermark.
  • Using base image: No
  • Aspect Ratio: auto

Celestial Navigator Under Starry Sky

• Model: DaVinci2

• Size: 2560 X 1456 (3.73 MP)

• Used settings:

  • Prompt: A celestial cartographer meticulously charts constellations on a parchment made of starlight, within a cosmic observatory. Nebulae swirl outside the crystalline dome, and constellations are depicted with glowing, intricate lines. The scene is bathed in soft, otherworldly light. Style of Moebius and James Gurney, with a touch of cosmic surrealism.
  • Using base image: No
  • Aspect Ratio: landscape_wide

Stars in the Vastness of the Night Sky

• Model: DaVinci2

• Size: 1152 X 864 (1.00 MP)

• Used settings:

  • Prompt: $$ \left[\frac{\partial}{\partial t}\,, \vec{\nabla}\right]\varphi=\frac{\partial}{\partial t}\left(\vec{\nabla}\varphi\right)-\vec{\nabla}\left(\frac{\partial \varphi}{\partial t}\right)\,\qquad\qquad\qquad\qquad \qquad(A1) $$ $$ \left[\frac{\partial}{\partial t}\,, \vec{\nabla}\cdot\right]\vec{F}=\frac{\partial}{\partial t}\left(\vec{\nabla}\cdot\vec{F}\right)-\vec{\nabla}\cdot\left(\frac{\partial \vec{F}}{\partial t}\right)\,\qquad \qquad\qquad\qquad (A2) $$ $$ \left[\frac{\partial}{\partial t}\,, \vec{\nabla}\times\right]\vec{F}=\frac{\partial}{\partial t}\left(\vec{\nabla}\times\vec{F}\right)-\vec{\nabla}\times\left(\frac{\partial \vec{F}}{\partial t}\right)\,\qquad\qquad\qquad\qquad (A3) $$ $$ \left[\frac{\partial}{\partial t}\,\,,\vec{\nabla}\times\right](\vec{F}\times\vec{G})=\vec{F}\times\left(\frac{\partial}{\partial t}(\vec{\nabla}\times\vec{G})-\vec{\nabla}\times\frac{\partial\vec{G}}{\partial t}\right)+\left(\vec{\nabla}\times\frac{\partial\vec{F}}{\partial t}-\frac{\partial}{\partial t}(\vec{\nabla}\times\vec{F})\right)\times\vec{G}\qquad (A4) $$ $$ \left[\frac{\partial}{\partial t}\,\,,\vec{\nabla}\right](\vec{F}\cdot\vec{G})=\vec{F}\left(\frac{\partial}{\partial t}(\vec{\nabla}\cdot\vec{G})-\vec{\nabla}\cdot\frac{\partial\vec{G}}{\partial t}\right)+\left(\vec{\nabla}\cdot\frac{\partial\vec{F}}{\partial t}-\frac{\partial}{\partial t}(\vec{\nabla}\cdot\vec{F})\right)\vec{G}\qquad\qquad\qquad\qquad (A5) $$ $$ \left[\frac{\partial^2}{\partial t^2}\,, \vec{\nabla}\right]\vec{\varphi}= \left[\frac{\partial}{\partial t}\,, \vec{\nabla}\right]\frac{\partial \varphi}{\partial t}\,, \left[\frac{\partial^2}{\partial t^2}\,, \vec{\nabla}\cdot\right]\vec{F}= \left[\frac{\partial}{\partial t}\,, \vec{\nabla\cdot}\right]\frac{\partial \vec{F}}{\partial t}\,, \left[\frac{\partial^2}{\partial t^2}\,, \vec{\nabla}\times\right]\vec{F}= \left[\frac{\partial}{\partial t}\,, \vec{\nabla\times}\right]\frac{\partial \vec{F}}{\partial t}\,(A6) $$ \end{document} If we now consider the interaction of a fermion particle with electromagnetic field ($A_\mu$), the spinor derivative will become \begin{equation} P'_\mu=p_\mu-eA'_\mu\,,\qquad A'_\mu=A_\mu-\frac{m_0c}{e}\,\gamma_\mu\,. \end{equation}
  • Using base image: No
  • Aspect Ratio: landscape