| 1. | That can be determined by evaluating the quadratic term of a divided difference formula.
|
| 2. | At high frequencies the quadratic term becomes important.
|
| 3. | Quadratic terms in and arise, which give masses to the W and Z bosons:
|
| 4. | Subtracting one equation from another eliminates these quadratic terms, leaving only the linear ones.
|
| 5. | Since each vibrational modes contributes to two quadratic terms in the Hamiltonian, you get:
|
| 6. | Partial pivoting adds only a quadratic term; this is not the case for full pivoting.
|
| 7. | The spatial symmetry of the problem is responsible for canceling the quadratic term of the expansion.
|
| 8. | In fact, this is the origin of the quadratic term in the field strength tensor.
|
| 9. | The same behavior can be obtained from the functional integrals, omitting the quadratic terms in the action.
|
| 10. | Lord Rayleigh investigated this first and quantified the magnetization M as a linear and quadratic term in the field:
|