Query about Grassmann Variables in Lewis Ryder's book

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maverick280857
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Query about Grassmann Variables a + b\eta

Hi,

What does

[tex]a + b\eta[/tex]

where a and b are c-numbers and [itex]\eta[/itex] is a Grassmann number, really mean?

At first sight, this does not seem like a valid thing to do, as this can't be interpreted as a regular composition and sum in Grassmann space -- there is no concept of an identity which could be 'multiplied' with a in the first term (and so the first term is a c-number, whereas the second is a scalar multiple of a Grassmann number).

And yet we do this all the time!
 
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From the mathematical point of view you simply defined the operation of sum and product of a Grassman number with C-numbers.

In physics that number can be interpred as the number resulting by the application of a sum of a bosonic and a fermionic destruction operators on the product of a bosonic and a fermionic coherent state:

[itex] \{a,a^\dagger \}=1 \, , \; [b,b ^\dagger ]=1 \, , \\<br /> |\eta \rangle = e^{-\eta a^\dagger} |0\rangle\, , \; |\phi \rangle = e^{ \phi b^\dagger} |0\rangle \, , \\<br /> \Rightarrow (a+ b)|\eta;\phi \rangle = (\phi + \eta)|\eta;\phi \rangle[/itex]

I know this was a stupid answer... but that's the best I can do now :smile:

Ilm
 
It's not more difficult than z=a+ib with z² = (a² - b²) + 2iab; replacing i by η and i²=-1 by η²=0 you arrive at Grassmann numbers
 
tom.stoer said:
It's not more difficult than z=a+ib with z² = (a² - b²) + 2iab; replacing i by η and i²=-1 by η²=0 you arrive at Grassmann numbers

I see your point. However, in writing z = a + ib, you are really writing

[tex]z = a \times \mathbb{1} + b \times i[/tex]

where [itex]\mathbb{1}[/itex] is an identity element of the space of complex numbers. Put another way, the first term [itex]a[/itex] is as much of a complex number as the second term [itex]ib[/itex], so adding them is like adding two elements of the same space.

However, with Grassmann numbers, you are effectively adding a c-number to a c-number multiple of a Grassmann number. When you do that, what is the entity you generate? (I realize that my question really points to the definition of '+'.) Is it a Grassmann number, or is it something else?

In other words, if [itex]\eta[/itex] is a Grassmann number (so [itex]\eta \in \mathcal{G}[/itex]), and I define

[tex]f(\eta) = a + b\eta[/tex]

where [itex]a, b \in \mathbb{C}[/itex] (i.e. a and b are c-numbers), is it correct to say that

[tex]f: \mathcal{G} \rightarrow \mathcal{G}[/tex]

?
 
I don't see you point; why not doing exatly the same with a*1 + b*η and 1²=1, η²=0? then 1 and η span a two-dim. vector space with an additional operation (a*1 + b*η)(c*1 + d*η) = ac*1 + (ad+bc)*η; it's purely formal but it works

In addition there is a matrix representation of Grassmann algebras http://en.wikipedia.org/wiki/Grassmann_number so it shouldn't really bother you
 
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