Why modulo m1 and modulo m2 implies modulo [m1, m2]

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If a ≡ r (mod m1) and a ≡ r (mod m2), then a must also satisfy a ≡ r (mod [m1, m2]). The proof begins by noting that if m1 divides (a - r) and m2 divides (a - r), then (a - r) is a common multiple of m1 and m2. Consequently, it follows that (a - r) is divisible by the least common multiple, [m1, m2]. This establishes that [m1, m2] divides (a - r), confirming the original statement. Thus, the relationship between the moduli is validated through their divisibility properties.
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Why "modulo m1" and "modulo m2" implies "modulo [m1, m2]"

If a \equiv r (mod m1) and a \equiv r (mod m2) then a \equiv r (mod [m1, m2]), where [a, b] is the least common multiple of a and b.

I have tried to prove that.

Assume that
[m_{1}, m_{2}] = l_{1}m_{1} = l_{2}m_{2}

and

a = k_{1}m_{1} + r
a = k_{2}m_{2} + r

Then

al_{1} = k_{1}l_{1}m_{1} + rl_{1}
al_{2} = k_{2}l_{2}m_{2} + rl_{2}

thus

a(l_{1} - l_{2}) = [m_{1}, m_{2}](k_{1} - k_{2}) + r(l_{1} - l_{2})

and

a = [m_{1}, m_{2}] {(k_{1} - k_{2}) \over (l_{1} - l_{2})} + r

In order to

a \equiv r\ (mod [m_{1}, m_{2}]), or a = K[m_{1}, m_{2}] + r

we have to prove that

(l_{1} - l_{2})\; | \; (k_{1} - k_{2})

But how?
 
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This doesn't directly answer your question, but wouldn't the proof be a lot easier if you started off with m1|(a-r) and m2|(a-r) ... ?
 


Gokul43201 said:
This doesn't directly answer your question, but wouldn't the proof be a lot easier if you started off with m1|(a-r) and m2|(a-r) ... ?

You are right, the proof is actually very simple:

If m1 | (a-r) and m2 | (a-r) then a-r is a common multiple of m1 and m2. Therefore it is divisible by the least common multiple, [m1, m2]. Thus [m1, m2] | (a-r), or a \equiv r (mod [m1, m2])
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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