Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 46279 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ | 0.5427 | 0.6866 | 0.7905 | [M:[0.7727, 1.1322, 0.9628], q:[0.2645, 0.9628], qb:[0.6033, 0.4339], phi:[0.4339]] | [M:[[11], [-2], [-7]], q:[[-4], [-7]], qb:[[6], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{3}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}^{4}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | -1 | t^2.095 + t^2.318 + t^2.603 + 2*t^2.888 + 2*t^3.397 + t^3.905 + 2*t^4.19 + t^4.413 + t^4.636 + 2*t^4.698 + t^4.922 + 2*t^4.983 + 2*t^5.207 + 3*t^5.492 + t^5.715 + 3*t^5.777 - t^6. + t^6.223 + 4*t^6.285 + t^6.731 + 3*t^6.793 + t^6.955 + t^7.017 + 3*t^7.078 + t^7.24 + t^7.302 + 2*t^7.525 + 4*t^7.587 + t^7.81 + 3*t^7.872 + t^8.033 + t^8.095 - 2*t^8.318 + 5*t^8.38 + t^8.541 - t^8.603 + 4*t^8.665 - 3*t^8.888 - t^4.302/y - t^6.62/y - t^7.19/y + (2*t^7.413)/y + t^7.698/y + t^7.922/y + (3*t^7.983)/y + (2*t^8.207)/y + (4*t^8.492)/y + (2*t^8.715)/y + t^8.777/y - t^8.938/y - t^4.302*y - t^6.62*y - t^7.19*y + 2*t^7.413*y + t^7.698*y + t^7.922*y + 3*t^7.983*y + 2*t^8.207*y + 4*t^8.492*y + 2*t^8.715*y + t^8.777*y - t^8.938*y | t^2.095/g1^3 + g1^11*t^2.318 + g1^2*t^2.603 + (2*t^2.888)/g1^7 + (2*t^3.397)/g1^2 + g1^3*t^3.905 + (2*t^4.19)/g1^6 + g1^8*t^4.413 + g1^22*t^4.636 + (2*t^4.698)/g1 + g1^13*t^4.922 + (2*t^4.983)/g1^10 + 2*g1^4*t^5.207 + (3*t^5.492)/g1^5 + g1^9*t^5.715 + (3*t^5.777)/g1^14 - t^6. + g1^14*t^6.223 + (4*t^6.285)/g1^9 + g1^19*t^6.731 + (3*t^6.793)/g1^4 + g1^33*t^6.955 + g1^10*t^7.017 + (3*t^7.078)/g1^13 + g1^24*t^7.24 + g1*t^7.302 + 2*g1^15*t^7.525 + (4*t^7.587)/g1^8 + g1^6*t^7.81 + (3*t^7.872)/g1^17 + g1^20*t^8.033 + t^8.095/g1^3 - 2*g1^11*t^8.318 + (5*t^8.38)/g1^12 + g1^25*t^8.541 - g1^2*t^8.603 + (4*t^8.665)/g1^21 - (3*t^8.888)/g1^7 - (g1*t^4.302)/y - (g1^12*t^6.62)/y - t^7.19/(g1^6*y) + (2*g1^8*t^7.413)/y + t^7.698/(g1*y) + (g1^13*t^7.922)/y + (3*t^7.983)/(g1^10*y) + (2*g1^4*t^8.207)/y + (4*t^8.492)/(g1^5*y) + (2*g1^9*t^8.715)/y + t^8.777/(g1^14*y) - (g1^23*t^8.938)/y - g1*t^4.302*y - g1^12*t^6.62*y - (t^7.19*y)/g1^6 + 2*g1^8*t^7.413*y + (t^7.698*y)/g1 + g1^13*t^7.922*y + (3*t^7.983*y)/g1^10 + 2*g1^4*t^8.207*y + (4*t^8.492*y)/g1^5 + 2*g1^9*t^8.715*y + (t^8.777*y)/g1^14 - g1^23*t^8.938*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|
| 46547 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$ + ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.5633 | 0.7261 | 0.7758 | [M:[0.7764, 1.1316, 0.9605, 0.6973], q:[0.2631, 0.9605], qb:[0.6053, 0.4342], phi:[0.4342]] | 2*t^2.092 + t^2.329 + t^2.605 + 2*t^2.881 + 2*t^3.395 + 4*t^4.184 + 2*t^4.421 + t^4.659 + 3*t^4.697 + t^4.935 + 4*t^4.973 + 2*t^5.211 + 5*t^5.487 + t^5.724 + 3*t^5.763 - 2*t^6. - t^4.303/y - t^4.303*y | detail |
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 45970 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.5429 | 0.6874 | 0.7898 | [M:[0.7766, 1.1258, 0.9719], q:[0.2674, 0.9561], qb:[0.6068, 0.4213], phi:[0.4371]] | t^2.066 + t^2.33 + t^2.623 + 2*t^2.916 + 2*t^3.377 + t^3.839 + 2*t^4.132 + t^4.396 + t^4.659 + 2*t^4.689 + t^4.952 + 2*t^4.982 + 2*t^5.245 + 2*t^5.443 + t^5.538 + t^5.707 + 3*t^5.831 + t^5.905 - 2*t^6. - t^4.311/y - t^4.311*y | detail |