Bound State of Heavy Quarks Using a General Polynomial Potential
Bound State of Heavy Quarks Using a General Polynomial Potential
In the present work, the mass spectra of the bound states of heavy quarks<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M1"><mml:mi mathvariant="normal">c</mml:mi><mml:mover accent="true"><mml:mrow><mml:mi mathvariant="normal">c</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:mover><mml:mo>,</mml:mo><mml:mi mathvariant="normal">b</mml:mi><mml:mover accent="true"><mml:mrow><mml:mi mathvariant="normal">b</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:mover></mml:math>, and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M2"><mml:mrow><mml:msub><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>meson are studied within the framework of the nonrelativistic Schrödinger’s equation. First, we solve Schrödinger’s equation with a general polynomial potential by Nikiforov-Uvarov (NU) method. The …