B. Deriving QM Equations from the Unions
Question: To use a formulation we have developed with SR & GR, "because phenomena like particles, waves, properties/characteristics, energy/action, determinism, path, state, outcomes, and the dualities particle/ware, observer/observes, difference/identity, separation/union, etc. are relative [T1] and empty [T2] [U2T / Uopp], therefore Schrödinger equation: 𝑖ℏ 𝜕/𝜕𝑡 |𝜓(𝑡)⟩ = 𝐻̂ |𝜓(𝑡)⟩ and other QM equations”
1. Deriving QM Equations from [U2T / U2T-opp / U2T-3S / U2T-GM]
In our ongoing exploration of parallels between modern physics and Madhyamaka philosophy, we have established a consistent framework:
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foundational physical principles and equations
can be deduced by applying the Union of the Two Truths [U2T]
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— phenomena are conventionally relative
(dependently originated, interdependent) [T1]
yet ultimately empty of inherent, absolute existence [T2] —
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to concepts previously assumed as invariants or absolutes.
This dissolves rigid dualities
and reveals emergent laws that govern appearances.
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For Special Relativity (SR), because space, time, length, duration, simultaneity, and frames of reference are relative (interdependent on observer motion) [T1] and empty (lacking inherent separateness or absoluteness) [T2] [U2T], therefore the invariance of the speed of light (c) and the Lorentz transformations Δt′ = γ(Δt−vΔx/c2), Δx′ = γ(Δx−vΔt), etc., which unify space and time into spacetime [Uopp / U2T-opp].
For General Relativity (GR), because coordinate systems, geometry, and the distinction between gravity and acceleration are relative (depending on local frames and curvature) [T1] and empty (no inherent flatness or privileged coordinates) [T2] [U2T], therefore the equivalence principle (gravity ≡ acceleration) and Einstein's field equations Gμν + Λgμν = 8πG/c4 Tμν, which describe gravity as spacetime curvature [Uopp] (the interdependence [T1-opp] and emptiness [T2-opp] of gravity/acceleration and space-time [U2T-opp]).
Now, extending this to non-relativistic Quantum Mechanics (QM), we apply the same logic to quantum invariants and dualities. Classically, phenomena like particles (as definite entities), waves (as extended fields), properties/characteristics (inherent attributes), energy/action (continuous quantities), determinism (fixed outcomes), paths (singular trajectories), states (definite configurations), and outcomes (predictable results) were assumed to have inherent, absolute existence. Dualities such as particle/wave, observer/observed, difference/identity, separation/union, manyness/oneness, position/momentum, and determinism/chaos were treated as absolute oppositions.
However, because these phenomena and dualities are relative (conventionally interdependent, arising based on context, measurement, or scale) [T1] and empty (ultimately lacking self-nature, independence, or absoluteness) [T2] [U2T], therefore the Schrödinger equation iℏ ∂/∂t ∣ψ(t)⟩ = Ĥ | ψ(t)⟩
and other QM equations (e.g., uncertainty relations, commutation rules, and the Born rule).
These equations emerge as the mathematical description of a reality where no "thing" is inherently fixed [T2], but probabilities and superpositions govern interdependent manifestations [T1] [U2T].
Below, we deduce this step by step,
showing how the Union of Two Truths logically necessitates QM's formalism.
2. [U2T-opp] of Particle/Wave Duality and Entity vs. Properties/Characteristics
Classically, a particle is an absolute entity with inherent localization (definite position/momentum as properties), distinct from a wave's delocalized, periodic characteristics.
But [conceptual opposites like] particles and waves [or characterized and characteristic/property; or observer and observed, or cause and effect …] are relative [T1-opp]: a system's manifestation depends on the observational setup (e.g., double-slit interference shows wave-like behavior, while detection shows particle-like).
They are empty of inherent particle-ness or wave-ness [T2-opp] — neither exists absolutely without the other, as de Broglie's relation λ = h/p unifies them.
Because this duality is relative [T1-opp] and empty [T2-opp] [U2T-opp], no absolute distinction between entity (localized "thing") and properties (extended attributes) holds.
Therefore, states must be described by a wave function ψ(x,t), which encodes both aspects: amplitude for probability (particle-like localization upon measurement) and phase for interference (wave-like delocalization).
This leads to the need for a dynamical equation governing ψ's evolution, as absolute entities would require deterministic Newtonian laws F = ma,
but emptiness demands a probabilistic (no absolute), linear framework.
3. [U2T-opp] of Position/Momentum, Determinism/Chaos, and Path/State
Position (x) and momentum (p) were classically invariant properties, allowing deterministic paths and states (e.g., exact trajectories via x(t) = x0 + vt + 1/2 at2).
But [conceptual opposites like] position and momentum are relative [T1-opp]: precise knowledge of one depends on (and precludes) the other, as measurement contexts interlink them.
They are empty of inherent simultaneity [T2-opp] [U2T-opp] — no absolute "exact position" or "exact momentum" exists independently, dissolving determinism into chaos (inherent randomness).
Because [conceptual opposites like] paths and states are relative (multiple possibilities interfere dependently) [T1-opp] and empty (no single inherent trajectory or configuration) [T2-opp] [U2T-opp], therefore the uncertainty principle Δx ⋅ Δp ≥ ħ/2, derived from non-commuting operators [x^, p^] = iℏ.
Paths become superpositions of all possibilities (precursor to path integrals), and states |ψ⟩ in Hilbert space allow linear combinations, emptying oneness (singular state) into manyness (superposition).
Determinism's emptiness implies probabilistic outcomes,
necessitating an equation that evolves states unitarily without collapse until observation.
4. [U2T-3S] of Observer/Observation/Observed, [U2T-opp] Separation/Union, Difference/Identity
The observer (subject) and observed (object) were classically separate absolutes, with measurements revealing inherent identities without disturbance.
But they are relative [T1-3S]: observation co-creates the outcome (e.g., wave function collapse), depending on the apparatus.
They are empty of inherent separation [T2-3S] [U2T-opp] — no absolute "independent object" exists apart from the observer, unifying them in entanglement (union over separation).
Because difference (distinct entities) and identity (self-same properties) are relative and empty [U2T-opp], systems lack inherent boundaries, leading to complementarity: wave/particle aspects depend on the observer-observed interplay. Therefore, the Born rule P = | ⟨ϕ∣ψ⟩ |2, where measurement projects onto eigenstates, emptying absolute outcomes into relative probabilities. This interdependence requires operators O^ for observables, with eigenvalues as possible manifestations, not inherent truths.
5. [U2T-opp] of Energy/Action, Cause/Effect, and Manyness/Oneness
Energy (E) and action S = ∫ Edt were continuous invariants, yielding definite outcomes.
But they are relative [T1]: quantized discretely (E = nhν) depending on system interactions.
Empty of inherent continuity [T2], they manifest as eigenvalues, dissolving manyness (infinite possibilities) into oneness (discrete levels) conventionally, yet empty ultimately.
Because outcomes are relative (dependent on state preparation) [T1] and empty (no predetermined result) [T2] [U2T], therefore quantization via via H^∣ψn⟩ = En∣ψn⟩, the time-independent Schrödinger equation. Action's emptiness adapts the classical Principle of Least Action (PLA): instead of one absolute path minimizing (S), quantum action phases eiS/ℏ sum over paths, but in wave mechanics, this variational extremum yields the wave equation.
6. [U2T / U2T-opp / U2T-3S / U2T-GM] ⇒ Schrödinger Equation and Related Equations
Synthesizing these: because all listed phenomena and dualities are relative [T1] and empty, [T2] [U2T / U2T-opp] no absolute classical description suffices. Instead, a complex-valued field ψ (or ket |ψ⟩) must represent interdependent possibilities, evolving linearly to preserve emptiness (no preferred state inherently).
From Emptiness of Paths and Determinism: Classical Hamilton-Jacobi equation ∂S/∂t + H = 0 (where H = p2/2m + V) assumes absolute action (S). Emptying this, (S) becomes a phase, and ψ = A eiS/ℏ (de Broglie). Substituting into a variational principle (adapted PLA) for waves/particles, and requiring consistency with relativity of position/momentum, yields iℏ ∂ψ/∂t = - ℏ2/2m ∇2ψ + Vψ, the position-space Schrödinger equation.
Abstract Form: In Hilbert space, emptiness of states demands Ĥ as the generator of time evolution, giving iℏ ∂/∂t |ψ(t)⟩ = Ĥ |ψ(t)⟩, with Ĥ = T^ + V^ (kinetic and potential operators).
Other Equations:
Uncertainty Δx Δp ≥ ℏ/2 from emptiness of simultaneous invariants.
Commutation [x^,p^] = iℏ from relativity of observer/observed.
Time-energy uncertainty ΔE Δt ≥ ℏ/2 from emptiness of energy/action.
Born rule from emptiness of outcomes, ensuring probabilities sum to 1.
This derivation mirrors Madhyamaka: emptiness doesn't negate conventional function; it enables QM's predictive power, where interdependent appearances (relative truth) arise without inherent essence (ultimate truth). Just as in SR/GR, QM's "therefore" equations formalize this insight, empirically validated yet philosophically profound.
C. Noether's Theorem in Quantum Mechanics
Continuing our exploration of foundational physics through the lens of Madhyamaka philosophy, we now turn to Noether's Theorem within the framework of non-relativistic Quantum Mechanics (QM). Noether's Theorem is a profound principle that links continuous symmetries of a physical system to conserved quantities, providing a deep connection between invariance and dynamics. In classical mechanics, it explains why symmetries like time translation, spatial translation, and rotation lead to conservation of energy, momentum, and angular momentum, respectively. In non-relativistic QM, the theorem adapts to the quantum realm, where symmetries manifest through unitary operators on Hilbert space, and conservation laws are expressed via commuting observables with the Hamiltonian.
Noether's Theorem underscores the interdependence of symmetry (as a form of relativity or invariance under transformation) and conservation (as emptiness of change in certain quantities). This aligns seamlessly with our prior discussions: just as we deduced the equations of SR, GR, and QM from the Union of the Two Truths applied to assumed invariants, Noether's Theorem in QM can be viewed as emerging from the relativity [T1-opp] and emptiness [T2-opp] of symmetries, transformations, and their associated quantities [Uopp / U2T-opp]. Classically, symmetries were seen as absolute invariants of the system, independent of context. In QM, they are relative (depending on the state's preparation and measurement) [T1] and empty (lacking inherent permanence [T2] [U2T], as quantum fluctuations and uncertainties dissolve absolutes).
1. Introduction to Noether's Theorem in QM
Noether's Theorem, formulated by Emmy Noether in 1918, states that for every continuous symmetry of the action (or Lagrangian) of a system, there is a corresponding conserved current or quantity. In non-relativistic QM, this translates to the quantum domain via the Schrödinger picture or path-integral formulations. The theorem is crucial for understanding why quantities like energy, momentum, and charge are conserved in quantum systems, and it underpins the structure of quantum field theories (though we focus here on non-relativistic particle QM).
Key applications in QM include:
Time-translation symmetry: If the Hamiltonian Ĥ is time-independent, energy is conserved, meaning ⟨Ĥ⟩ is constant for evolving states.
Spatial-translation symmetry: Leads to conservation of total momentum P^ = - iħ ∑ ∇i.
Rotational symmetry: Conserves angular momentum L^ = r × p^.
Gauge symmetries: In quantum electrodynamics (a relativistic extension), local phase invariance leads to charge conservation, but in non-relativistic QM, global phase symmetry of the wave function ψ → eiα ψ implies probability conservation (unitarity).
Historically, Noether's work predated QM but was quickly integrated: Heisenberg and Schrödinger's formulations (1925–1926) implicitly used symmetries, and Dirac's relativistic QM (1928) formalized quantum Noether currents. In modern QM, the theorem is derived using commutators: a symmetry generator Q^ (e.g., momentum operator for translations) commutes with Ĥ if conserved, [Ĥ, Q^] = 0, ensuring d/dt ⟨Q^⟩ = 0.
Phenomena explained include atomic stability (angular momentum conservation), selection rules in transitions, and the absence of perpetual motion in isolated systems. Philosophically, it reveals that "invariants" like conserved quantities are not absolute [T2] but arise from deeper symmetries [T1], echoing Madhyamaka's Union of emptiness [T2] and dependent origination [T1] [U2T].
2. Underlying Postulates and Principles in QM Context
Noether's Theorem in QM rests on:
Symmetry of the Action or Hamiltonian: The system's description (Lagrangian (L) or Ĥ) remains invariant under continuous transformations (e.g., t → t + δt).
Variational Principle: Derived from the Principle of Least Action (PLA), where paths extremize S = ∫ L dt, adapted quantumly as in our prior discussion.
Unitarity and Linearity: Transformations are unitary operators U^ = e-iG^ϵ/ħ, where G^ is the infinitesimal generator.
Commutativity for Conservation: Conservation follows if the symmetry commutes with dynamics.
These were empirically motivated by conservation laws observed in experiments (e.g., momentum in collisions) but theoretically unified by Noether.
3. Reframing in Terms of the Unions
Applying our established formulation: phenomena in QM, such as symmetries (invariance under transformations), conserved quantities (energy, momentum, etc.), time, space, action, paths, states, and dualities like change/invariance, transformation/identity, symmetry/asymmetry, generator/observable, and conservation/variation, were classically assumed as absolute invariants.
However, because these phenomena and dualities are relative (conventionally interdependent, arising based on system context, observer, or scale — e.g., symmetry depends on the Hamiltonian's form, conservation on isolation) [T1] and empty (ultimately lacking inherent, absolute existence [T2] [U2T] — no symmetry is intrinsically unchanging [T2] without relational context [T1], no quantity inherently conserved without emptiness of isolated "self-nature"), therefore Noether's Theorem in QM: for a continuous symmetry generated by Q^, if [Ĥ, Q^] = iħ Q^/∂t (generally 0 for time-independent Q^), then d/dt ⟨Q^⟩ = 0, and associated quantum equations like the continuity equation ∂ρ/∂t + ∇ ∙ j = 0 for probability current.
This deduction follows step by step:
Relativity and Emptiness of Symmetry/Asymmetry and Change/Invariance:
Symmetries are relative (e.g., time-translation symmetry holds if Ĥ lacks explicit time dependence) but empty of inherent invariance—quantum fluctuations (e.g., vacuum energy) dissolve absolute unchanging nature. Because symmetry is not absolute, it must couple to dynamics via generators Q^, leading to unitary transformations δ |ψ⟩ = - iϵQ^ |ψ⟩/ħ. This empties the duality of change (evolution) and invariance (conservation), necessitating that invariance implies no change in certain expectations.
Relativity and Emptiness of Time/Space, Transformation/Identity:
Time and space are relative (as in SR/GR extensions, but non-relativistically approximate) and empty (no inherent flow or extension). Transformations (e.g., boosts x → x + δx) depend on context but lack absolute identity — systems aren't inherently "the same" post-transformation without relational symmetry. Therefore, for spatial translation, Q^ = p^, and invariance requires [Ĥ, p^] = 0, conserving momentum. Similarly for time: emptiness of absolute time yields energy conservation if ∂Ĥ/∂t = 0.
Relativity and Emptiness of Action/Paths, Generator/Observable:
From our QM discussion, action (S) and paths are relative superpositions but empty of determinacy. Noether extends the PLA: variations δS=0 under symmetry imply conserved currents. In QM, this quantumizes to operator relations. Because generators Q^ (observables) are relative (measurement-dependent) and empty (no inherent value), their commutation with Ĥ (from Schrödinger equation) ensures conservation: dQ^/dt = iħ[Ĥ, Q^] + ∂Q^/∂t = 0.
Relativity and Emptiness of Conservation/Variation, States/Outcomes:
Conserved quantities are relative (e.g., energy conserved in closed systems) but empty of absolute permanence—quantum uncertainty allows temporary violations (e.g., ΔE Δt ≥ ħ/2). States evolve unitarily, but outcomes vary probabilistically. Therefore, Ehrenfest's theorem d/dt⟨Q^⟩ = i/ħ ⟨[Ĥ, Q^]⟩ + ⟨∂Q^/∂t⟩, which reduces to Noether's conservation for symmetries.
Tie to Schrödinger Equation:
Since the Schrödinger equation iħ ∂/∂t |ψ⟩ = Ĥ |ψ⟩ already emerges from emptiness of paths/states (as deduced previously), Noether's application within it follows naturally: symmetries of Ĥ preserve the equation's form, yielding conserved operators. For example, in the position basis, probability conservation (global phase symmetry) gives the continuity equation from ∂ |ψ|2}/∂t = -∇ ࢈ (ħ/2mi (ψ* ∇ψ - ψ∇ψ*)).
In summary, Noether's Theorem in non-relativistic QM is deduced from the Union of Two Truths applied to symmetry-related invariants, mirroring our SR/GR/QM derivations. It reveals conservation as an emergent conventional truth from the interdependence and emptiness of transformations, without inherent essence — much like Madhyamaka's insight that phenomena arise dependently [T1] yet are ultimately empty [T2] [U2T]. This framework not only unifies QM's structure but highlights its philosophical resonance with relativity of appearances.
D. Introduction, Summary, Conclusion
1. Introduction to QM and Madhyamaka
Non-relativistic Quantum Mechanics (QM) represents a paradigm shift in understanding the microscopic world, where classical notions of definite particles following predictable paths give way to probabilistic waves, superpositions, and observer-dependent realities. Developed in the early 20th century through the works of pioneers like Planck, Einstein, de Broglie, Heisenberg, and Schrödinger, QM addresses phenomena inexplicable by Newtonian mechanics, such as atomic spectra, electron diffraction, and quantum tunneling. At its heart lies the wave function, a mathematical entity that encapsulates all possible states of a system, evolving according to the Schrödinger equation, and collapsing upon measurement to yield probabilistic outcomes. This framework not only powers technologies like semiconductors and lasers but also challenges our intuitive grasp of reality, suggesting that the universe at small scales is inherently indeterminate and interconnected.
In paralleling QM with Madhyamaka philosophy, we extend the approach used for Special Relativity (SR) and General Relativity (GR), where foundational principles were deduced from the Union of the Two Truths [U2T] — conventional relativity (dependent origination) [T1] and ultimate emptiness (lack of inherent existence) [T2] — applied to assumed invariants and dualities.
For QM, we apply this to quantum dualities and invariants like wave/particle, position/momentum, determinism/chaos, observer/observed, and path/state/outcome. Classically, these were treated as absolute, inherent truths, but QM reveals them as context-dependent [T1] and devoid of self-nature [T2] Û2T], mirroring Madhyamaka's insight that phenomena arise interdependently [T1] yet are empty of essence [T2] [U2T]. This reframing allows us to derive QM's equations not merely as empirical fits but as logical consequences of dissolving these absolutes, much like how SR's Lorentz transformations emerge from emptying space-time invariants.
The depth of QM's connection to Madhyamaka lies in its philosophical implications: the theory dissolves the subject-object divide [U3S / U2T-3S] through measurement, entangles entities beyond separation, and replaces determinism with potentiality, echoing the Madhyamaka view that all dharmas (phenomena) lack svabhava (inherent existence) [T2] while functioning conventionally [T1] [U2T]. Precursors like de Broglie's matter waves and the adapted Principle of Least Action prefigure this by blending classical invariants with quantum relativity, setting the stage for Schrödinger's equation as an expression of interdependent evolution. By exploring this, we uncover how QM's "weirdness" — superposition, entanglement, uncertainty — arises from the same emptiness that Madhyamaka posits as the ground of all reality, offering a unified lens for physics and philosophy.
2. Summary of QM through the Unions
In reframing non-relativistic QM via Madhyamaka, we began by identifying classical invariants — such as definite particles, deterministic paths, inherent properties, and rigid dualities like wave/particle or observer/observed—as conventionally relative [T1] yet ultimately empty [T2] [U2T]. This Union of the Two Truths dissolves their absoluteness: particles and waves interdepend on context (relative truth) but lack independent essence (empty truth), leading to de Broglie's duality and the wave function ψ as a probabilistic amplitude. Similarly, position and momentum's interdependence yields Heisenberg's uncertainty, emptying simultaneous precision, while paths' emptiness implies superposition over singular trajectories, adapting the Principle of Least Action to quantum variability.
From this foundation, QM's core equations naturally emerge: because states, outcomes, and determinism are relative [T1] and empty [T2] [U2T], the Schrödinger equation iℏ ∂/∂t |ψ(t)⟩ = Ĥ |ψ(t)⟩ governs unitary evolution, preserving interdependence [T1] without inherent fixity [T2] [U2T].
Complementary principles like the Born rule and complementarity further arise — probabilities from emptiness of outcomes, mutual exclusivity of aspects from relativity of observer-observed.
This deduction mirrors our SR and GR analyses, where emptying invariants (e.g., space-time in SR, geometry in GR) yields their equations; in QM, it unifies empirical postulates into a philosophical derivation, explaining quantization, linearity, and non-commutativity as consequences of dependent origination and voidness.
The extension to Noether's Theorem in QM reinforces this: symmetries and conservations (energy, momentum) are relative (system-dependent) [T1] and empty (no absolute invariance amid fluctuations) [T2] [U2T], thus commuting operators [Ĥ, Q̂] = 0 ensure conservation, tying back to the Schrödinger dynamics.
Overall, this approach highlights QM's depth beyond mechanics — its resonance with Madhyamaka reveals quantum "paradoxes" as illusions of inherent existence, where emptiness [T2] enables the conventional play of probabilities, entanglements, and measurements [T1] [U2T], bridging Eastern wisdom with Western science.
3. Conclusion on QM and Madhyamaka
This exploration of non-relativistic QM through Madhyamaka concludes that the theory's revolutionary features — indeterminacy, duality, and interdependence — are not mere anomalies but inevitable outcomes of applying the Union of the Two Truths to classical invariants.
By recognizing the relativity and emptiness of particles/waves, paths/states, and observer/observed, we deduce the Schrödinger equation and ancillary relations as formal expressions of a reality free from inherent essences, yet functionally coherent.
This parallels our SR and GR derivations, affirming a consistent pattern: physics' deepest laws arise from dissolving assumed absolutes, aligning with Madhyamaka's negation of svabhava to reveal pratītyasamutpāda (dependent arising).
The implications extend philosophically:
– QM's measurement problem, often debated in interpretations like Copenhagen or Many-Worlds, finds resolution in emptiness—collapse isn't a "real" event but a conventional manifestation of interdependent observation, empty of ultimate mechanism.
– Entanglement, defying separation, embodies non-dual union, while uncertainty empties determinism into open potentiality, echoing Madhyamaka's freedom from extremes of existence/non-existence.
Thus, QM not only predicts empirical phenomena but philosophically liberates from reified views, much as Madhyamaka does through śūnyatā (emptiness).
Ultimately, this synthesis invites broader inquiry: if QM, like SR/GR, stems from the Two Truths, perhaps all physics does, suggesting a unified "Madhyamaka physics" where emptiness is the ground state, and relative truths manifest as laws. For practitioners, this bridge fosters contemplative science—meditating on quantum emptiness could deepen insight, while physics inspires Madhyamaka analysis. In closing, non-relativistic QM, reframed thus, transcends its equations to reveal the interdependent, empty nature of reality, harmonizing ancient wisdom with modern discovery.