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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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Quantum cosmology with self–<strong>in</strong>teract<strong>in</strong>g scalar field 197<br />

prime are <strong>de</strong>rivatives with respect to The Hamiltonian can be constructed<br />

<strong>and</strong> we expressed it as S<strong>in</strong>ce N is a Lagrange multiplier,<br />

we have the constra<strong>in</strong>t <strong>and</strong> follow the Dirac quantization<br />

procedure this equation is known as WDW equation. This<br />

equation is <strong>in</strong><strong>de</strong>pen<strong>de</strong>nt of N , however <strong>in</strong> the follow<strong>in</strong>g we use the<br />

gauges N = 1 <strong>and</strong> s<strong>in</strong>ce we obta<strong>in</strong> simpler equations with<br />

those choices.<br />

2.1. GAUGE N=1<br />

With the choice N = 1, the action (5) becomes<br />

hence the canonical conjugate momenta correspond<strong>in</strong>g to <strong>and</strong> <strong>and</strong><br />

the correspond<strong>in</strong>g Hamiltonian can be calculated<br />

now, the canonical momenta <strong>in</strong> Eq. (7) are converted <strong>in</strong>to operators <strong>in</strong><br />

the st<strong>and</strong>ard way, <strong>and</strong> the ambiguity<br />

of factor or<strong>de</strong>r<strong>in</strong>g is enco<strong>de</strong>d <strong>in</strong> the parameter The result<strong>in</strong>g WDW<br />

equation is<br />

Next we present three simple solvable cases for different cosmological<br />

terms.<br />

Case The solution to WDW equation without a<br />

cosmological term <strong>and</strong> is<br />

where is a separation constant, the Bessel function or<strong>de</strong>r is given by<br />

By superposition of the above solutions we obta<strong>in</strong>

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