Quantum Consepts - that can be wrong-but Usually ain't

 https://closedlooppulsepropulsion.com/Verdict_Token/ https://verdict-frontend.fly.dev/ https://verdict-api.fly.dev/ https://github.com/mikelewis1971/verdict_token I decided to fix the consensus coin, mainly becuase it sort of sucked.  The idea was that you mint coins and consensus is reached when you burn them all.  There's no monetary value but I did charge 1 polygon for the service.  It's like 25 cents to use that smart contract.  While it worked... it's not really what I wanted... So I created a new token called Verdict Token.  You create x amount of tokens and you can specify y number of burned coins as the votes needed to reach an onchain immutable concensus.  The idea is that if you tie these coins to a smart contract, you can only change things that are agreed on by the coin holders.  This is the DAO coin that you always wanted. I cleaned it up and locked it in at 25 cent  U.S. per contract so it's cheap.  You give me 25 cents an...

  It's a simple coin.   You mint as many as you want.  You pass them out and when they're all burned, consensus is reached.  Because it's on the Polygon network, fees are cheap and the minimum is 1 Pol which is .25 cents to validate any vote by consensus.   Simple mechanics... print tokens.  Consensus is met when all are burned.  No questions, no games.  Want to unlock an LP?  Burn all the tokens and you can.  https://github.com/mikelewis1971/ConsensusCoin This is the github page... try it out.  It's cheap and useful.  I have to use it to create my next coin so I hope you get a chance to try it out. 

  Below is a math-only, citation-rich derivation of two canonical “geometric–drift” effects: Berry phase – a quantum‐mechanical geometric phase that appears when a system’s parameters trace a closed loop. Stokes drift – the net Lagrangian mass transport that appears in an oscillatory fluid even though its Eulerian mean velocity is zero. The calculations show how each effect arises from a higher-order term (curvature for Berry; quadratic wave amplitude for Stokes) and why, despite superficial similarities, they live in different branches of mechanics. 1 Berry phase: geometric phase from the Legendre map 1.1 Setup and adiabatic gauge Let ∣ n ( R ) ⟩ \lvert n(\mathbf R)\rangle ∣ n ( R )⟩ be an instantaneous, non-degenerate eigenstate H ( R ) ∣ n ( R ) ⟩ = E n ( R ) ∣ n ( R ) ⟩ , R ( t ) ∈ M , H(\mathbf R)\lvert n(\mathbf R)\rangle =E_n(\mathbf R)\lvert n(\mathbf R)\rangle,\qquad \mathbf R(t)\in\mathcal M , H ( R ) ∣ n ( R )⟩ = E n ​ ( R ) ∣ n ( R )⟩ , R ( t )...