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Physlib.Particles.FlavorPhysics.CKMMatrix.PhaseFreedom

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theorem

u+d=arg(Vud)u + d = -\arg(V_{ud}) implies Vud=VudV'_{ud} = |V_{ud}| under phase rephasing

#shift_ud_phase_zero

Let VV be a 3×33 \times 3 unitary CKM matrix. Let VV' be the matrix obtained by applying row phase shifts (u,c,t)(u, c, t) and column phase shifts (d,s,b)(d, s, b) to VV such that V=(eiu000eic000eit)V(eid000eis000eib) V' = \begin{pmatrix} e^{iu} & 0 & 0 \\ 0 & e^{ic} & 0 \\ 0 & 0 & e^{it} \end{pmatrix} V \begin{pmatrix} e^{id} & 0 & 0 \\ 0 & e^{is} & 0 \\ 0 & 0 & e^{ib} \end{pmatrix} where u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R}. If the phase parameters uu and dd satisfy the condition u+d=arg(Vud)u + d = -\arg(V_{ud}), then the udud-entry (the element at row 0 and column 0) of the transformed matrix VV' is real and equal to the absolute value Vud|V_{ud}|.

theorem

The VusV_{us} element becomes Vus|V_{us}| under phase rotation if u+s=arg(Vus)u + s = -\arg(V_{us})

#shift_us_phase_zero

Let VV be a 3×33 \times 3 unitary CKM matrix and let u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R} be real phase parameters. If the sum of the phase parameters uu and ss satisfies the condition u+s=arg(Vus)u + s = -\arg(V_{us}), then the entry in the first row and second column of the phase-shifted matrix V=diag(eiu,eic,eit)Vdiag(eid,eis,eib)V' = \text{diag}(e^{iu}, e^{ic}, e^{it}) \cdot V \cdot \text{diag}(e^{id}, e^{is}, e^{ib}) is equal to the absolute value Vus|V_{us}|. Here arg(Vus)\arg(V_{us}) denotes the phase of the complex matrix element VusV_{us} in the first row and second column.

theorem

Vub=VubV'_{ub} = |V_{ub}| under phase shift u+b=arg(Vub)u + b = -\arg(V_{ub})

#shift_ub_phase_zero

Let VV be a CKM matrix (a 3×33 \times 3 unitary matrix). Suppose we apply a phase shift transformation to VV using six real parameters u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R} to obtain a new matrix VV': V=(eiu000eic000eit)V(eid000eis000eib) V' = \begin{pmatrix} e^{iu} & 0 & 0 \\ 0 & e^{ic} & 0 \\ 0 & 0 & e^{it} \end{pmatrix} V \begin{pmatrix} e^{id} & 0 & 0 \\ 0 & e^{is} & 0 \\ 0 & 0 & e^{ib} \end{pmatrix} If the parameters uu and bb satisfy the condition u+b=arg(Vub)u + b = -\arg(V_{ub}), where VubV_{ub} is the matrix element in the first row and third column, then the corresponding element of the transformed matrix is real and equal to the absolute value of the original element, i.e., Vub=VubV'_{ub} = |V_{ub}|.

theorem

Phase shift c+s=arg(Vcs)c + s = -\arg(V_{cs}) implies Vcs=VcsV'_{cs} = |V_{cs}|

#shift_cs_phase_zero

Let VV be a 3×33 \times 3 unitary CKM matrix. Consider a phase shift transformation of VV parameterized by six real numbers u,c,tu, c, t (corresponding to rows) and d,s,bd, s, b (corresponding to columns), resulting in a new matrix VV' defined as: V=(eiu000eic000eit)V(eid000eis000eib) V' = \begin{pmatrix} e^{iu} & 0 & 0 \\ 0 & e^{ic} & 0 \\ 0 & 0 & e^{it} \end{pmatrix} V \begin{pmatrix} e^{id} & 0 & 0 \\ 0 & e^{is} & 0 \\ 0 & 0 & e^{ib} \end{pmatrix} If the phase parameters cc and ss satisfy the condition c+s=arg(Vcs)c + s = -\arg(V_{cs}), where VcsV_{cs} is the entry of VV at row index 1 and column index 1, then the entry VcsV'_{cs} of the transformed matrix is equal to the absolute value of the original entry, i.e., Vcs=VcsV'_{cs} = |V_{cs}|.

theorem

Vcb=VcbV'_{cb} = |V_{cb}| when c+b=arg(Vcb)c + b = -\arg(V_{cb})

#shift_cb_phase_zero

Let VV be a 3×33 \times 3 unitary CKM matrix. Let VV' be the matrix obtained by applying phase shifts to the rows and columns of VV with real parameters u,c,tu, c, t (for the rows) and d,s,bd, s, b (for the columns), defined by V=diag(eiu,eic,eit)Vdiag(eid,eis,eib)V' = \text{diag}(e^{iu}, e^{ic}, e^{it}) V \text{diag}(e^{id}, e^{is}, e^{ib}). If the phase parameters cc and bb satisfy the condition c+b=arg(Vcb)c + b = -\arg(V_{cb}), then the entry in the second row and third column of the transformed matrix is real and equal to the magnitude of the original entry, i.e., Vcb=VcbV'_{cb} = |V_{cb}|.

theorem

Vtb=VtbV'_{tb} = |V_{tb}| when t+b=arg(Vtb)t + b = -\arg(V_{tb})

#shift_tb_phase_zero

Let VV be a 3×33 \times 3 unitary CKM matrix and let u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R} be real phase parameters. Let VV' be the transformed matrix obtained by: V=diag(eiu,eic,eit)Vdiag(eid,eis,eib) V' = \text{diag}(e^{iu}, e^{ic}, e^{it}) \cdot V \cdot \text{diag}(e^{id}, e^{is}, e^{ib}) If the parameters tt and bb satisfy the condition t+b=arg(Vtb)t + b = -\arg(V_{tb}), where arg(Vtb)\arg(V_{tb}) is the phase of the entry in the third row and third column, then the tbtb entry of the transformed matrix is real and equal to the absolute value of the original entry, i.e., Vtb=VtbV'_{tb} = |V_{tb}|.

theorem

Phase Shift Condition for Vcd=VcdV'_{cd} = -|V_{cd}|

#shift_cd_phase_pi

Let VV be a 3×33 \times 3 unitary CKM matrix. For any six real phase parameters u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R}, let VV' be the transformed CKM matrix obtained by: V=diag(eiu,eic,eit)Vdiag(eid,eis,eib) V' = \text{diag}(e^{iu}, e^{ic}, e^{it}) \cdot V \cdot \text{diag}(e^{id}, e^{is}, e^{ib}) where ii is the imaginary unit. If the phase parameters cc and dd satisfy the condition c+d=πarg(Vcd)c + d = \pi - \arg(V_{cd}), then the entry of the transformed matrix in the charm row and down column satisfies: Vcd=Vcd V'_{cd} = -|V_{cd}| where arg(Vcd)\arg(V_{cd}) is the phase of the original matrix element VcdV_{cd} and Vcd|V_{cd}| is its absolute value.

theorem

Phase Shift Condition for Vt=(Vu)×(Vc)\mathbf{V}'_t = (\mathbf{V}'_u)^* \times (\mathbf{V}'_c)^*

#shift_cross_product_phase_zero

Let VV be a CKM matrix, which is a 3×33 \times 3 unitary matrix. Let Vu,Vc,VtC3\mathbf{V}_u, \mathbf{V}_c, \mathbf{V}_t \in \mathbb{C}^3 denote the first, second, and third rows of VV respectively (corresponding to the up, charm, and top quarks). Suppose there exists a real number τ\tau such that the rows satisfy the relation eiτ(Vu×Vc)=Vte^{i\tau} (\mathbf{V}_u^* \times \mathbf{V}_c^*) = \mathbf{V}_t, where V\mathbf{V}^* denotes the component-wise complex conjugate and ×\times denotes the cross product in C3\mathbb{C}^3. Given six real phase parameters u,c,t,d,s,bRu, c, t, d, s, b \in \mathbb{R}, let VV' be the transformed CKM matrix obtained by: V=diag(eiu,eic,eit)Vdiag(eid,eis,eib) V' = \text{diag}(e^{iu}, e^{ic}, e^{it}) \cdot V \cdot \text{diag}(e^{id}, e^{is}, e^{ib}) If the parameters satisfy the condition τ=(u+c+t+d+s+b)\tau = -(u + c + t + d + s + b), then the rows of the transformed matrix VV' satisfy: Vt=(Vu)×(Vc) \mathbf{V}'_t = (\mathbf{V}'_u)^* \times (\mathbf{V}'_c)^* where ii is the imaginary unit.

definition

Condition for non-negative real Vud,Vus,Vcb,VtbV_{ud}, V_{us}, V_{cb}, V_{tb} and row relation Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*

#FstRowThdColRealCond

For a CKM matrix UU, which is a 3×33 \times 3 complex unitary matrix with entries VijV_{ij} (i{u,c,t}i \in \{u, c, t\}, j{d,s,b}j \in \{d, s, b\}), this proposition holds if the matrix elements VudV_{ud}, VusV_{us}, VcbV_{cb}, and VtbV_{tb} are equal to their absolute values (and are thus non-negative real numbers), and the third row vector Vt\mathbf{V}_t is equal to the cross product of the complex conjugates of the first row Vu\mathbf{V}_u and the second row Vc\mathbf{V}_c, expressed as: Vud=Vud,Vus=Vus,Vcb=Vcb,Vtb=Vtb V_{ud} = |V_{ud}|, \quad V_{us} = |V_{us}|, \quad V_{cb} = |V_{cb}|, \quad V_{tb} = |V_{tb}| and Vt=Vu×Vc \mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^* where V\mathbf{V}^* denotes the element-wise complex conjugate and ×\times denotes the standard cross product in C3\mathbb{C}^3.

definition

Phase condition for Vub=1|V_{ub}| = 1 and Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*

#ubOnePhaseCond

For a CKM matrix UU, represented as a 3×33 \times 3 complex unitary matrix with entries VijV_{ij} (i{u,c,t}i \in \{u, c, t\}, j{d,s,b}j \in \{d, s, b\}), this proposition holds if: 1. The matrix elements VudV_{ud}, VusV_{us}, and VcbV_{cb} are 00. 2. The matrix element VubV_{ub} is equal to 11. 3. The third row vector Vt\mathbf{V}_t is equal to the cross product of the complex conjugates of the first row Vu\mathbf{V}_u and the second row Vc\mathbf{V}_c: Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^* where V\mathbf{V}^* denotes the element-wise complex conjugate and ×\times denotes the standard cross product in C3\mathbb{C}^3. 4. The matrix elements VcdV_{cd} and VcsV_{cs} are real and satisfy Vcd=VcdV_{cd} = -|V_{cd}| and Vcs=1Vcd2V_{cs} = \sqrt{1 - |V_{cd}|^2}, where Vcd|V_{cd}| is the absolute value of the VcdV_{cd} entry.

theorem

Solution for Phase Shift Equations in CKM Matrices

#fstRowThdColRealCond_shift_solution

Let VV be a CKM matrix, represented as a 3×33 \times 3 complex unitary matrix, with entries VijV_{ij} where i{u,c,t}i \in \{u, c, t\} and j{d,s,b}j \in \{d, s, b\}. Suppose a,b,c,d,e,fa, b, c, d, e, f, and τ\tau are real parameters satisfying the following system of linear equations based on the arguments (phases) of specific matrix elements: 1. a+d=arg(Vud)a + d = -\arg(V_{ud}) 2. a+e=arg(Vus)a + e = -\arg(V_{us}) 3. b+f=arg(Vcb)b + f = -\arg(V_{cb}) 4. c+f=arg(Vtb)c + f = -\arg(V_{tb}) 5. τ=(a+b+c+d+e+f)\tau = -(a + b + c + d + e + f) Then the variables b,c,d,e,b, c, d, e, and ff are uniquely determined by a,τ,a, \tau, and the phases of VV as follows: - b=τ+arg(Vud)+arg(Vus)+arg(Vtb)+ab = -\tau + \arg(V_{ud}) + \arg(V_{us}) + \arg(V_{tb}) + a - c=τ+arg(Vcb)+arg(Vud)+arg(Vus)+ac = -\tau + \arg(V_{cb}) + \arg(V_{ud}) + \arg(V_{us}) + a - d=arg(Vud)ad = -\arg(V_{ud}) - a - e=arg(Vus)ae = -\arg(V_{us}) - a - f=τarg(Vud)arg(Vus)arg(Vcb)arg(Vtb)af = \tau - \arg(V_{ud}) - \arg(V_{us}) - \arg(V_{cb}) - \arg(V_{tb}) - a

theorem

Solution for the phase shift parameters under the `ubOnePhaseCond` for a CKM matrix

#ubOnePhaseCond_shift_solution

Let VV be a CKM matrix, and let a,b,c,d,e,fa, b, c, d, e, f be real numbers representing phase shifts. If these parameters satisfy the system of equations: 1. a+f=argVuba + f = -\arg V_{ub} 2. a+b+c+d+e+f=0a + b + c + d + e + f = 0 3. b+d=πargVcdb + d = \pi - \arg V_{cd} 4. b+e=argVcsb + e = -\arg V_{cs} Then the parameters are related by: - c=argVcd+argVcs+argVub+bπc = \arg V_{cd} + \arg V_{cs} + \arg V_{ub} + b - \pi - d=πargVcdbd = \pi - \arg V_{cd} - b - e=argVcsbe = -\arg V_{cs} - b - f=argVubaf = -\arg V_{ub} - a

theorem

Any CKM matrix is equivalent to one satisfying `FstRowThdColRealCond`

#fstRowThdColRealCond_holds_up_to_equiv

For any 3×33 \times 3 unitary CKM matrix VV, there exists a CKM matrix UU that is equivalent to VV under phase rephasing (VUV \approx U) and satisfies the condition `FstRowThdColRealCond`. Two matrices V,UV, U are equivalent if there exist real parameters a,b,c,d,e,fRa, b, c, d, e, f \in \mathbb{R} such that U=diag(eia,eib,eic)Vdiag(eid,eie,eif). U = \text{diag}(e^{ia}, e^{ib}, e^{ic}) V \text{diag}(e^{id}, e^{ie}, e^{if}). The condition `FstRowThdColRealCond` is satisfied for UU if the matrix elements Vud,Vus,VcbV_{ud}, V_{us}, V_{cb}, and VtbV_{tb} are non-negative real numbers (i.e., Vij=VijV_{ij} = |V_{ij}|) and the third row vector Vt\mathbf{V}_t is equal to the cross product of the complex conjugates of the first row Vu\mathbf{V}_u and the second row Vc\mathbf{V}_c: Vt=Vu×Vc. \mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*.

theorem

Existence of an Equivalent CKM Matrix satisfying `ubOnePhaseCond` when Vub=1|V_{ub}| = 1

#ubOnePhaseCond_hold_up_to_equiv_of_ub_one

Let VV be a 3×33 \times 3 unitary CKM matrix that satisfies the condition `FstRowThdColRealCond` (meaning VudV_{ud}, VusV_{us}, VcbV_{cb}, and VtbV_{tb} are non-negative real numbers and the row vectors satisfy Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*). If Vud=0V_{ud} = 0 and Vus=0V_{us} = 0 (which, for a unitary matrix, implies Vub=1|V_{ub}| = 1), then there exists a CKM matrix UU equivalent to VV under phase rephasing (VUV \approx U) such that UU satisfies the `ubOnePhaseCond`. Specifically, UU satisfies the following: 1. Uud=0U_{ud} = 0, Uus=0U_{us} = 0, and Ucb=0U_{cb} = 0. 2. Uub=1U_{ub} = 1. 3. The third row vector Ut\mathbf{U}_t is the cross product of the complex conjugates of the first two rows: Ut=Uu×Uc\mathbf{U}_t = \mathbf{U}_u^* \times \mathbf{U}_c^*. 4. The remaining charm-row elements are real and satisfy Ucd=UcdU_{cd} = -|U_{cd}| and Ucs=1Ucd2U_{cs} = \sqrt{1 - |U_{cd}|^2}.

theorem

Formula for VcdV_{cd} under the `FstRowThdColRealCond` phase convention

#cd_of_fstRowThdColRealCond

Let VV be a 3×33 \times 3 unitary CKM matrix. Suppose VV satisfies the condition `FstRowThdColRealCond`, which implies that the matrix elements VudV_{ud}, VusV_{us}, VcbV_{cb}, and VtbV_{tb} are non-negative real numbers, and the third row vector is given by the cross product of the complex conjugates of the first two rows, Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*. If Vud0V_{ud} \neq 0 or Vus0V_{us} \neq 0, then the matrix element VcdV_{cd} is given by: Vcd=VtbVus+VubVudVcbeiarg(Vub)Vud2+Vus2V_{cd} = -\frac{|V_{tb}| |V_{us}| + |V_{ub}| |V_{ud}| |V_{cb}| e^{-i \arg(V_{ub})}}{|V_{ud}|^2 + |V_{us}|^2} where Vij|V_{ij}| denotes the absolute value of the entry in the ii-th row and jj-th column, and arg(Vub)\arg(V_{ub}) is the phase of the element VubV_{ub}.

theorem

Vcs=VtbVudVubVusVcbeiargVubVud2+Vus2V_{cs} = \frac{|V_{tb}| |V_{ud}| - |V_{ub}| |V_{us}| |V_{cb}| e^{-i \arg V_{ub}}}{|V_{ud}|^2 + |V_{us}|^2} under `FstRowThdColRealCond` phase convention

#cs_of_fstRowThdColRealCond

Let VV be a 3×33 \times 3 unitary CKM matrix with entries VijV_{ij} for i{u,c,t}i \in \{u, c, t\} and j{d,s,b}j \in \{d, s, b\}. Suppose that Vud0V_{ud} \neq 0 or Vus0V_{us} \neq 0. If VV satisfies the condition `FstRowThdColRealCond` (meaning that the matrix elements Vud,Vus,VcbV_{ud}, V_{us}, V_{cb}, and VtbV_{tb} are non-negative real numbers and the third row vector Vt\mathbf{V}_t is the cross product of the complex conjugates of the first two rows, Vt=Vu×Vc\mathbf{V}_t = \mathbf{V}_u^* \times \mathbf{V}_c^*), then the matrix element VcsV_{cs} is given by: Vcs=VtbVudVubVusVcbeiargVubVud2+Vus2V_{cs} = \frac{|V_{tb}| |V_{ud}| - |V_{ub}| |V_{us}| |V_{cb}| e^{-i \arg V_{ub}}}{|V_{ud}|^2 + |V_{us}|^2} where Vij|V_{ij}| denotes the magnitude of the matrix element and argVub\arg V_{ub} denotes the phase of VubV_{ub}.