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 |
|---|---|---|---|---|---|---|---|---|---|
| 3951 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ | 0.6395 | 0.7939 | 0.8055 | [X:[1.6178], M:[0.8533, 0.6756, 1.1467, 0.3822, 0.8089, 0.7645, 1.1911], q:[0.4044, 0.7423], qb:[0.4489, 0.8755], phi:[0.3822]] | [X:[[4]], M:[[12], [-28], [-12], [-4], [2], [-8], [-2]], q:[[1], [-13]], qb:[[11], [17]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}$ | -2 | t^2.027 + 2*t^2.293 + t^2.56 + t^3.44 + 2*t^3.573 + 2*t^3.84 + t^4.054 + 2*t^4.32 + 4*t^4.587 + 3*t^4.853 + t^5.12 + t^5.467 + 2*t^5.6 + t^5.733 + 4*t^5.867 - 2*t^6. + t^6.081 + 4*t^6.133 - t^6.267 + 2*t^6.347 + 2*t^6.4 + 4*t^6.614 + 7*t^6.88 + 6*t^7.147 - 2*t^7.28 + 3*t^7.413 + t^7.494 - 2*t^7.546 + 2*t^7.627 + 3*t^7.68 + t^7.76 + 4*t^7.894 - t^8.027 + t^8.108 + 6*t^8.16 - 5*t^8.293 + 2*t^8.374 + 6*t^8.427 - 6*t^8.56 + 4*t^8.641 + 4*t^8.693 - 2*t^8.826 + 7*t^8.907 + 2*t^8.96 - t^4.147/y - t^6.174/y - (2*t^6.44)/y + (2*t^7.32)/y + (2*t^7.587)/y + (4*t^7.853)/y + t^8.12/y - t^8.2/y - t^8.467/y + (2*t^8.6)/y - t^8.733/y + (6*t^8.867)/y - t^4.147*y - t^6.174*y - 2*t^6.44*y + 2*t^7.32*y + 2*t^7.587*y + 4*t^7.853*y + t^8.12*y - t^8.2*y - t^8.467*y + 2*t^8.6*y - t^8.733*y + 6*t^8.867*y | t^2.027/g1^28 + (2*t^2.293)/g1^8 + g1^12*t^2.56 + t^3.44/g1^12 + (2*t^3.573)/g1^2 + 2*g1^18*t^3.84 + t^4.054/g1^56 + (2*t^4.32)/g1^36 + (4*t^4.587)/g1^16 + 3*g1^4*t^4.853 + g1^24*t^5.12 + t^5.467/g1^40 + (2*t^5.6)/g1^30 + t^5.733/g1^20 + (4*t^5.867)/g1^10 - 2*t^6. + t^6.081/g1^84 + 4*g1^10*t^6.133 - g1^20*t^6.267 + (2*t^6.347)/g1^64 + 2*g1^30*t^6.4 + (4*t^6.614)/g1^44 + (7*t^6.88)/g1^24 + (6*t^7.147)/g1^4 - 2*g1^6*t^7.28 + 3*g1^16*t^7.413 + t^7.494/g1^68 - 2*g1^26*t^7.546 + (2*t^7.627)/g1^58 + 3*g1^36*t^7.68 + t^7.76/g1^48 + (4*t^7.894)/g1^38 - t^8.027/g1^28 + t^8.108/g1^112 + (6*t^8.16)/g1^18 - (5*t^8.293)/g1^8 + (2*t^8.374)/g1^92 + 6*g1^2*t^8.427 - 6*g1^12*t^8.56 + (4*t^8.641)/g1^72 + 4*g1^22*t^8.693 - 2*g1^32*t^8.826 + (7*t^8.907)/g1^52 + 2*g1^42*t^8.96 - t^4.147/(g1^4*y) - t^6.174/(g1^32*y) - (2*t^6.44)/(g1^12*y) + (2*t^7.32)/(g1^36*y) + (2*t^7.587)/(g1^16*y) + (4*g1^4*t^7.853)/y + (g1^24*t^8.12)/y - t^8.2/(g1^60*y) - t^8.467/(g1^40*y) + (2*t^8.6)/(g1^30*y) - t^8.733/(g1^20*y) + (6*t^8.867)/(g1^10*y) - (t^4.147*y)/g1^4 - (t^6.174*y)/g1^32 - (2*t^6.44*y)/g1^12 + (2*t^7.32*y)/g1^36 + (2*t^7.587*y)/g1^16 + 4*g1^4*t^7.853*y + g1^24*t^8.12*y - (t^8.2*y)/g1^60 - (t^8.467*y)/g1^40 + (2*t^8.6*y)/g1^30 - (t^8.733*y)/g1^20 + (6*t^8.867*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3682 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.6555 | 0.8217 | 0.7977 | [X:[1.6173], M:[0.8518, 0.6792, 1.1482, 0.3827, 0.8086, 0.7655], q:[0.4043, 0.7439], qb:[0.4475, 0.8734], phi:[0.3827]] | t^2.037 + 2*t^2.296 + t^2.426 + t^2.555 + t^3.445 + t^3.574 + 2*t^3.833 + t^4.075 + 2*t^4.334 + t^4.463 + 4*t^4.593 + 2*t^4.722 + 4*t^4.852 + t^4.981 + t^5.111 + t^5.482 + t^5.612 + t^5.741 + 3*t^5.871 - t^6. - t^4.148/y - t^4.148*y | detail |