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Given the Schrödinger equation:

$$-\frac { { \hbar }^{ 2 } }{ 2m } \frac { { d }^{ 2 } }{ { dx }^{ 2 } } \Psi +V(x)\Psi =E\Psi $$

What does $-\cfrac { { \hbar }^{ 2 } }{ 2m } \cfrac { { d }^{ 2 } }{ { dx }^{ 2 } } $ represent?

A

The kinetic energy operator.

B

The potential energy operator.

C

The Hamiltonian operator.

D

The eigenvalue.

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