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An operator form of the 3N bound state is proposed. It consists of eightoperators formed out of scalar products in relative momentum and spin vectors,which are applied on a pure 3N spin 1/2 state. Each of the operators isassociated with a scalar function depending only on the magnitudes of the tworelative momenta and the angle between them. The connection between thestandard partial wave decomposition of the 3N bound state and the operator formis established, and the decomposition of these scalar function in terms ofpartial wave components and analytically known auxiliary functions is given.That newly established operator form of the 3N bound state exhibits thedominant angular and spin dependence analytically. The scalar functions aretabulated and can be downloaded. As an application the spin dependent nucleonmomentum distribution in a polarized 3N bound state is calculated to illustratethe use of the new form of the 3N bound state.Comment: 21 pages, 1 table, 8 figures, revtex

physical review. c. nuclear physics/physical review. c, nuclear physics

Operator form of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">H</mml:mi><mml:mprescripts /><mml:none /><mml:mn>3</mml:mn></mml:mmultiscripts></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mmultiscripts><mml:mi mathvariant="normal">He</mml:mi><mml:mprescripts /><mml:none /><mml:mn>3</mml:mn></mml:mmultiscripts><mml:mo>)</mml:mo></mml:mrow></mml:math>…

Operator form ofH3(He3)…