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The general solution is any linear combination of these two.
Therefore, the only possible way to get a linear combination is with these coefficients.
One can work with more familiar variables as linear combinations of these.
For example, may be one or more linear combinations of .
The coefficients or weights of the linear combination can be learned as well.
The final wave function is a linear combination of these two functions.
To do this, one must add all powers of "X" and their linear combinations as well.
This is known as a linear combination of experts.
So a solution on the edge can be written as a linear combination of plane waves.
The portfolio itself is assumed to be some linear combination of these instruments.
The general state in a Fock space is a linear combination of pure states.
The new position can then be expressed as a linear combination of the search vectors.
Whether the other linear combinations are useful is a different matter, but one cannot just throw away possible solutions "without cause".
Not too surprisingly the math gives the result that there are exactly four such linear combinations!
Statistical mixtures of states are separate from a linear combination.
This means that any state can be written as a linear combination of the basis spinors.
Conditions 2 and 3 for a subspace are simply the most basic kinds of linear combinations.
The set of all possible linear combinations is called the span:
Products are linear combinations of the periods, and he determines the coefficients.
The source data (8x8) is transformed to a linear combination of these 64 frequency squares.
If two time series and are cointegrated, a linear combination of them must be stationary.
Unlike the linear combination case each system is in a definite eigenstate.
The quantum states in the system can be described as linear combination of these eight states.
From here, the values of can be determined by linear combination (addition and/or subtraction).
This superposition or linear combination is called the Fourier series.