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 |
|---|---|---|---|---|---|---|---|---|---|
| 3879 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}X_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6724 | 0.8509 | 0.7902 | [X:[1.3318], M:[0.7153, 0.8094, 0.6682, 0.8565, 1.1435, 0.7153, 0.8094], q:[0.88, 0.4047], qb:[0.4518, 0.7388], phi:[0.3812]] | [X:[[28]], M:[[-18], [2], [-28], [12], [-12], [-18], [2]], q:[[17], [1]], qb:[[11], [-13]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | -1 | 2*t^2.146 + t^2.287 + 2*t^2.428 + t^2.569 + t^3.431 + t^3.713 + t^3.995 + 3*t^4.292 + 2*t^4.433 + 5*t^4.574 + 4*t^4.715 + 5*t^4.856 + 2*t^4.998 + t^5.139 + 2*t^5.576 + 2*t^5.859 - t^6. + 2*t^6.141 + t^6.282 + 2*t^6.424 + 4*t^6.437 + t^6.565 + 3*t^6.579 + 8*t^6.72 + 8*t^6.861 + 10*t^7.002 + 7*t^7.144 + 6*t^7.285 + 3*t^7.426 + t^7.708 + 3*t^7.722 + t^7.991 + 3*t^8.005 - 4*t^8.146 + t^8.287 - 6*t^8.428 + t^8.569 + 5*t^8.583 + 4*t^8.724 + 4*t^8.852 + 11*t^8.866 + 2*t^8.993 - t^4.144/y - (2*t^6.289)/y - t^6.431/y - (2*t^6.572)/y + t^7.292/y + (2*t^7.433)/y + (4*t^7.574)/y + (6*t^7.715)/y + (3*t^7.856)/y + (4*t^7.998)/y - (3*t^8.435)/y - (4*t^8.718)/y + (2*t^8.859)/y - t^4.144*y - 2*t^6.289*y - t^6.431*y - 2*t^6.572*y + t^7.292*y + 2*t^7.433*y + 4*t^7.574*y + 6*t^7.715*y + 3*t^7.856*y + 4*t^7.998*y - 3*t^8.435*y - 4*t^8.718*y + 2*t^8.859*y | (2*t^2.146)/g1^18 + t^2.287/g1^8 + 2*g1^2*t^2.428 + g1^12*t^2.569 + t^3.431/g1^12 + g1^8*t^3.713 + g1^28*t^3.995 + (3*t^4.292)/g1^36 + (2*t^4.433)/g1^26 + (5*t^4.574)/g1^16 + (4*t^4.715)/g1^6 + 5*g1^4*t^4.856 + 2*g1^14*t^4.998 + g1^24*t^5.139 + (2*t^5.576)/g1^30 + (2*t^5.859)/g1^10 - t^6. + 2*g1^10*t^6.141 + g1^20*t^6.282 + 2*g1^30*t^6.424 + (4*t^6.437)/g1^54 + g1^40*t^6.565 + (3*t^6.579)/g1^44 + (8*t^6.72)/g1^34 + (8*t^6.861)/g1^24 + (10*t^7.002)/g1^14 + (7*t^7.144)/g1^4 + 6*g1^6*t^7.285 + 3*g1^16*t^7.426 + g1^36*t^7.708 + (3*t^7.722)/g1^48 + g1^56*t^7.991 + (3*t^8.005)/g1^28 - (4*t^8.146)/g1^18 + t^8.287/g1^8 - 6*g1^2*t^8.428 + g1^12*t^8.569 + (5*t^8.583)/g1^72 + (4*t^8.724)/g1^62 + 4*g1^32*t^8.852 + (11*t^8.866)/g1^52 + 2*g1^42*t^8.993 - t^4.144/(g1^4*y) - (2*t^6.289)/(g1^22*y) - t^6.431/(g1^12*y) - (2*t^6.572)/(g1^2*y) + t^7.292/(g1^36*y) + (2*t^7.433)/(g1^26*y) + (4*t^7.574)/(g1^16*y) + (6*t^7.715)/(g1^6*y) + (3*g1^4*t^7.856)/y + (4*g1^14*t^7.998)/y - (3*t^8.435)/(g1^40*y) - (4*t^8.718)/(g1^20*y) + (2*t^8.859)/(g1^10*y) - (t^4.144*y)/g1^4 - (2*t^6.289*y)/g1^22 - (t^6.431*y)/g1^12 - (2*t^6.572*y)/g1^2 + (t^7.292*y)/g1^36 + (2*t^7.433*y)/g1^26 + (4*t^7.574*y)/g1^16 + (6*t^7.715*y)/g1^6 + 3*g1^4*t^7.856*y + 4*g1^14*t^7.998*y - (3*t^8.435*y)/g1^40 - (4*t^8.718*y)/g1^20 + (2*t^8.859*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3394 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}X_{1}$ | 0.6565 | 0.8232 | 0.7974 | [X:[1.336], M:[0.7126, 0.8097, 0.664, 0.8583, 1.1417, 0.7126], q:[0.8825, 0.4049], qb:[0.4534, 0.7369], phi:[0.3806]] | 2*t^2.138 + t^2.283 + t^2.429 + t^2.575 + t^3.425 + t^3.571 + t^3.717 + t^4.008 + 3*t^4.276 + 2*t^4.421 + 3*t^4.567 + 3*t^4.713 + 3*t^4.858 + t^5.004 + t^5.15 + 2*t^5.563 + 2*t^5.709 + 2*t^5.854 - t^4.142/y - t^4.142*y | detail |