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Autothermal syngas generation by combining simultaneous autothermal reforming in an air/oxygen-fired fixed-bed reactor (ATR) and steam reforming in a gas-heated tubular fixed-bed reactor (GHR) [32, 33].

The quantum counterpart of this reads as H in = a a + 1 2 H pert = a a + 1 2 F0 (a + a ) (104)



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The coherent states corresponding to the shifted parabola retain a Gaussian shape (eg, in position representation and up to a phase factor), the same as for the original ground state Now, one can explore the consequences of adding, at the classical level, a quadratic term to the potential: H in = p2 1 p2 1 + m 2 x 2 H pert = + m 2 x 2 F 0 ( g 1 x g 2 x 2 ) 2m 2 2m 2 (105)

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This actually amounts, besides the shifting of the parabola, to modifying the spring constant as k k = k + 2g 2 F 0 (106)

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On the quantum level, the Hamiltonian changes as H in = (a a + 1 ) H pert = (a a + 1 ) + P 2 (aa ) , 2 2 (107)

where P 2 is quadratic polynomial Then, the original ground state |0 changes into a kind of squeezed state, for which we now give a mathematical de nition De nition 101 A squeezed (coherent) state | , , , C, results from the combined action on the Fock vacuum state of the two following unitary operators: | , = D ( ) S( )|0 , D ( ) = e a

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S( ) = e 2 (

a a2 )

McGovern, J.; Bothner, P.; Cagle, K.; Linn, J.; Nagarajan, V. XQuery Kick Start Sams Publishing, March 2003 Ray, E. Learning XML O Reilly & Associates, February 2001

(108)

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