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 |
|---|---|---|---|---|---|---|---|---|---|
| 6385 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ + ${ }M_{5}M_{9}$ | 0.6704 | 0.8348 | 0.8031 | [M:[0.9683, 0.8153, 0.9683, 0.8153, 1.1847, 0.7388, 1.1847, 1.1082, 0.8153], q:[0.624, 0.4077], qb:[0.4077, 0.777], phi:[0.4459]] | [M:[[-22], [-2], [-22], [-2], [2], [8], [2], [12], [-2]], q:[[23], [-1]], qb:[[-1], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{2}$, ${ }M_{9}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{9}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{9}$, ${ }M_{3}M_{9}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{6}M_{7}$, ${ }M_{2}M_{8}$, ${ }M_{8}M_{9}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}M_{2}M_{7}$, ${ }M_{7}M_{9}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | -1 | t^2.216 + 2*t^2.446 + 2*t^2.905 + t^3.325 + t^3.554 + 2*t^3.784 + t^4.203 + 3*t^4.433 + 2*t^4.662 + 3*t^4.892 + t^5.082 + 2*t^5.121 + 2*t^5.351 + t^5.541 + 3*t^5.77 + 3*t^5.81 - t^6. + 4*t^6.23 + t^6.42 + t^6.459 + 3*t^6.649 + 2*t^6.689 + 4*t^6.879 + 3*t^7.108 + t^7.298 + 6*t^7.338 + 2*t^7.528 + 4*t^7.567 + 2*t^7.757 + 2*t^7.797 + 3*t^7.987 + 3*t^8.026 + 2*t^8.216 + 3*t^8.256 + t^8.406 - 3*t^8.446 + 2*t^8.636 + 5*t^8.675 + 4*t^8.715 + 4*t^8.866 - 5*t^8.905 - t^4.338/y - t^6.554/y - t^6.784/y - (2*t^7.243)/y + (2*t^7.433)/y + (2*t^7.662)/y + (2*t^7.892)/y + (3*t^8.121)/y + (4*t^8.351)/y + t^8.541/y + (2*t^8.77)/y + t^8.81/y - t^4.338*y - t^6.554*y - t^6.784*y - 2*t^7.243*y + 2*t^7.433*y + 2*t^7.662*y + 2*t^7.892*y + 3*t^8.121*y + 4*t^8.351*y + t^8.541*y + 2*t^8.77*y + t^8.81*y | g1^8*t^2.216 + (2*t^2.446)/g1^2 + (2*t^2.905)/g1^22 + g1^12*t^3.325 + g1^2*t^3.554 + (2*t^3.784)/g1^8 + g1^26*t^4.203 + 3*g1^16*t^4.433 + 2*g1^6*t^4.662 + (3*t^4.892)/g1^4 + g1^40*t^5.082 + (2*t^5.121)/g1^14 + (2*t^5.351)/g1^24 + g1^20*t^5.541 + 3*g1^10*t^5.77 + (3*t^5.81)/g1^44 - t^6. + (4*t^6.23)/g1^10 + g1^34*t^6.42 + t^6.459/g1^20 + 3*g1^24*t^6.649 + (2*t^6.689)/g1^30 + 4*g1^14*t^6.879 + 3*g1^4*t^7.108 + g1^48*t^7.298 + (6*t^7.338)/g1^6 + 2*g1^38*t^7.528 + (4*t^7.567)/g1^16 + 2*g1^28*t^7.757 + (2*t^7.797)/g1^26 + 3*g1^18*t^7.987 + (3*t^8.026)/g1^36 + 2*g1^8*t^8.216 + (3*t^8.256)/g1^46 + g1^52*t^8.406 - (3*t^8.446)/g1^2 + 2*g1^42*t^8.636 + (5*t^8.675)/g1^12 + (4*t^8.715)/g1^66 + 4*g1^32*t^8.866 - (5*t^8.905)/g1^22 - t^4.338/(g1^6*y) - (g1^2*t^6.554)/y - t^6.784/(g1^8*y) - (2*t^7.243)/(g1^28*y) + (2*g1^16*t^7.433)/y + (2*g1^6*t^7.662)/y + (2*t^7.892)/(g1^4*y) + (3*t^8.121)/(g1^14*y) + (4*t^8.351)/(g1^24*y) + (g1^20*t^8.541)/y + (2*g1^10*t^8.77)/y + t^8.81/(g1^44*y) - (t^4.338*y)/g1^6 - g1^2*t^6.554*y - (t^6.784*y)/g1^8 - (2*t^7.243*y)/g1^28 + 2*g1^16*t^7.433*y + 2*g1^6*t^7.662*y + (2*t^7.892*y)/g1^4 + (3*t^8.121*y)/g1^14 + (4*t^8.351*y)/g1^24 + g1^20*t^8.541*y + 2*g1^10*t^8.77*y + (t^8.81*y)/g1^44 |
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4790 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.6549 | 0.8078 | 0.8107 | [M:[0.9717, 0.8156, 0.9717, 0.8156, 1.1844, 0.7376, 1.1844, 1.1063], q:[0.6205, 0.4078], qb:[0.4078, 0.7766], phi:[0.4468]] | t^2.213 + t^2.447 + 2*t^2.915 + t^3.319 + 2*t^3.553 + 2*t^3.787 + t^4.191 + 3*t^4.425 + t^4.659 + t^4.894 + t^5.063 + 2*t^5.128 + t^5.532 + 3*t^5.766 + 3*t^5.83 - t^6. - t^4.341/y - t^4.341*y | detail |