Identifying the Bolch sphere with the Riemann sphere(the extended complex plane), we obtain relations between single qubit unitary operations and M\"{o}bius transformations on the extended complex plane.
We generalise our previous results of universal linear manipulations [Phys. Rev. A63, 032304 (2001)] to investigate three types of nonlinear qubit transformations using measurement and quantum based schemes. Firstly, nonlinear rotations are studied. We rotate different parts of a Bloch sphere in opposite directions about the z-axis. The second transformation is a map which sends a qubit to its orthogonal state (which we define as ORTHOG). We consider the case when the ORTHOG is applied to only a partial area of a Bloch sphere. We also study nonlinear general transformation, i.e. (theta,phi)->(theta-alpha,phi), again, applied only to part of the Bloch sphere. In order to achieve these three operations, we consider different measurement preparations and derive the optimal average (instead of universal) quantum unitary transformations. We also introduce a simple method for a qubit measurement and its application to other cases.
Abstract A pure state of a qubit can be geometrically represented as a point on the extended complex plane through stereographic projection. By employing successive conformal maps on the extended complex plane, we can generate an effective discrete-time evolution of the pure states of the qubit. This work focuses on a subset of analytic maps known as fractional linear conformal maps. We show that these maps serve as a unifying framework for a diverse range of quantum-inspired conceivable dynamics, including (i) unitary dynamics,(ii) non-unitary but linear dynamics and (iii) non-unitary and non-linear dynamics where linearity (non-linearity) refers to the action of the discrete time evolution operator on the Hilbert space. We provide a characterization of these maps in terms of Leggett–Garg inequality complemented with no-signaling in time and arrow of time conditions.
FINDING: Stereographic projection maps the Bloch sphere (quantum state space) to the complex plane, revealing a projective geometry where the golden ratio emerges as the fixed-point ratio of the Möbius transformation linking antipodal qubit states. | MATH: Stereographic projection: π(x1,x2,x3)=1−x3x1+ix2 for sphere S2→C∪{∞}. Bloch sphere: ∣ψ⟩=cos(θ/2)∣0⟩+eiϕsin(θ/2)∣1⟩. Möbius transformation on the Riemann sphere: z↦cz+daz+b, ad−bc=0. Cross-ratio invariance: (z1−z4)(z2−z3)(z1−z3)(z2−z4) is preserved under Möbius maps. For antipodal points z and −1/zˉ, the cross-ratio with {0,1,∞} yields the golden ratio φ=(1+5)/2≈1.618 when z=eiπ/5 (or its conjugate), satisfying z2−z−1=0 in the projective coordinate. | CONNECTION: The golden ratio \( \va Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
In this paper the geometry of two and three-qubit states under local unitary groups is discussed. We first review the one qubit geometry and its relation with Riemannian sphere under the action of group SU(2). We show that the quaternionic stereographic projection intertwines between local unitary group SU(2)⊗SU(2) and quaternionic Möbius transformation. The invariant term appearing in this operation is related to concurrence measure. Yet, there exists the same intertwining stereographic projection for much more global group Sp(2), generalizing the familiar Bloch sphere in 2-level systems. Subsequently, we introduce octonionic stereographic projection and octonionic conformal map (or octonionic Möbius maps) for three-qubit states and find evidence that they may have invariant terms under local unitary operations which shows that both maps are entanglement sensitive.