Template:Pictures in quantum mechanics

Nowadays, Template:Pictures in quantum mechanics is a topic that has gained great relevance in society. With the advancement of technology and access to information, more and more people are interested in learning about Template:Pictures in quantum mechanics and its implications in today's world. Whether from a historical, scientific, or cultural approach, Template:Pictures in quantum mechanics has captured the imagination of people of all ages and backgrounds. In this article, we will explore some key aspects of Template:Pictures in quantum mechanics, from its origins to its current impact, with the aim of shedding light on a topic that continues to be the subject of debate and reflection today.

Evolution of:	Picture ( v t e )
	Schrödinger (S)	Heisenberg (H)	Interaction (I)
Ket state	${\displaystyle |\psi _{\rm {S}}(t)\rangle =e^{-iH_{\rm {S}}~t/\hbar }|\psi _{\rm {S}}(0)\rangle }$	constant	${\displaystyle |\psi _{\rm {I}}(t)\rangle =e^{iH_{0,\mathrm {S} }~t/\hbar }|\psi _{\rm {S}}(t)\rangle }$
Observable	constant	${\displaystyle A_{\rm {H}}(t)=e^{iH_{\rm {S}}~t/\hbar }A_{\rm {S}}e^{-iH_{\rm {S}}~t/\hbar }}$	${\displaystyle A_{\rm {I}}(t)=e^{iH_{0,\mathrm {S} }~t/\hbar }A_{\rm {S}}e^{-iH_{0,\mathrm {S} }~t/\hbar }}$
Density matrix	${\displaystyle \rho _{\rm {S}}(t)=e^{-iH_{\rm {S}}~t/\hbar }\rho _{\rm {S}}(0)e^{iH_{\rm {S}}~t/\hbar }}$	constant	${\displaystyle \rho _{\rm {I}}(t)=e^{iH_{0,\mathrm {S} }~t/\hbar }\rho _{\rm {S}}(t)e^{-iH_{0,\mathrm {S} }~t/\hbar }}$