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Mathematics Notation using LATEX query

iℏ∂∂t|Ψ(t)⟩=H|Ψ(t)⟩i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right>=H\left|\Psi(t)\right>

i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right>=H\left|\Psi(t)\right>$

For inline math (inside a paragraph):

The time-dependent Schrödinger equation is ( i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right\rangle = H\left|\Psi(t)\right\rangle ).

(iℏ∂∂t|Ψ(t)⟩=H|Ψ(t)⟩)( i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right\rangle = H\left|\Psi(t)\right\rangle )

Jeremies work focussed on ( A_n ) this.

(An) ( A_n )

For display math (centered and on its own line):

[iℏ∂∂t|Ψ(t)⟩=H|Ψ(t)⟩][ i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right\rangle = H\left|\Psi(t)\right\rangle ]

[ i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right\rangle = H\left|\Psi(t)\right\rangle ]

Abstract: In this talk, we will first introduce flat fully augmented links… complement in $S^3$. … subgroups of $O(3)$ … $L_i$ … $Sym^{+}(\mathbb{S}^{3}, L_i) \cong Sym^{+}(\mathbb{S}^{3} \setminus L_i) \cong G$.

Abstract:Inthistalk,wewillfirstintroduceflatfullyaugmentedlinks,aclassofhyperboliclinkswhosecomplementsadmitparticularlytractablegeometricstructures.Wewillthendiscusshowa3−connected,planar,cubicgraphcalledacrushtaceanencodesmany,andsometimesall,oftheorientation−preservingsymmetriesofaflatfullyaugmentedlinkanditscomplementinS3.Abstract: In this talk, we will first introduce flat fully augmented links, a class of hyperbolic links whose complements admit particularly tractable geometric structures. We will then discuss how a 3-connected, planar, cubic graph called a crushtacean encodes many, and sometimes all, of the orientation-preserving symmetries of a flat fully augmented link and its complement in S^{3}.

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