Differential modulo another differential

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SUMMARY

The discussion centers on the concept of an odd derivation d being a differential modulo another differential d', defined by two conditions: [d, d'] = 0 and d^2 = -[d', d"] for some d". The first condition establishes that d acts as a derivative on H*(d'), while the second condition confirms that d is nilpotent in H*(d'). Participants reference the book "Quantization of Gauge Systems" by Henneaux and Teitelboim for further insights, particularly chapter 8, page 173, to clarify these concepts.

PREREQUISITES
  • Understanding of differential operators in algebraic topology
  • Familiarity with the concepts of homology and cohomology groups
  • Knowledge of BRST quantization techniques
  • Basic principles of gauge theories
NEXT STEPS
  • Study the implications of the commutator [d, d'] = 0 in differential geometry
  • Explore the concept of nilpotent operators in the context of differential forms
  • Review the derivation of H*(d') and its properties in algebraic topology
  • Investigate the BRST formalism and its applications in quantum field theory
USEFUL FOR

Mathematicians, physicists, and students specializing in algebraic topology, gauge theories, and quantum field theory will benefit from this discussion, particularly those interested in the properties of differential operators and their applications in BRST quantization.

astros
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Hello,

One says that an odd derivation d is a differential modulo another differential d' if this two things hold:

[d,d']=0
d^2=-[d',d"] for some d"

- The first condition says that d defines a derivative on H*(d'), but how? To have a well-defined action of this derivation on H*(d') we must have:
dx belongs to H*(d') whenever x belongs to H*(d') i.e: d'(dx)=0 & dx#d'y for every y
- d'(dx)=-dd'x=0 OK
- How to show the second one?

- The second condition says that d is indeed a differential i.e: d^2=0 in H*(d') but for x belongs to H*(d') we have:
d^2x=-d'd"x-d"d'x=-d'd"x ?, How does it vanish?
Thanks for every help...
 
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Off-topic: do you study BRST ?

On-topic, see the book of Henneaux and Teitelboim "Quantization of gauge systems", chapter # 8, page # 173.
 
Hi,
Yes I'm studying BRST
This book is precisely what I read now but I did not understand this section!
The problem is how the derivation d becomes a derivation on H*(d') by means of the first condition? an after that becomes nilpotent by means of the seconde condition?
 

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