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 |
|---|---|---|---|---|---|---|---|---|---|
| 58684 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{1}M_{8}$ | 0.6951 | 0.8533 | 0.8147 | [M:[1.0433, 0.974, 0.9567, 1.0087, 1.026, 0.974, 1.0087, 0.9567], q:[0.5043, 0.4524], qb:[0.5216, 0.539], phi:[0.4957]] | [M:[[10], [-6], [-10], [2], [6], [-6], [2], [-10]], q:[[1], [-11]], qb:[[5], [9]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{8}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$ | ${}$ | -4 | 2*t^2.87 + 2*t^2.922 + 2*t^3.026 + t^3.182 + t^4.201 + t^4.357 + t^4.409 + t^4.461 + t^4.513 + t^4.565 + 2*t^4.617 + t^4.669 + t^4.721 + 2*t^5.74 + 3*t^5.792 + 2*t^5.844 + 3*t^5.896 + 2*t^5.948 - 4*t^6. + 2*t^6.052 + t^6.104 - t^6.156 + t^6.208 - t^6.26 + t^6.364 + 2*t^7.071 + 2*t^7.123 + 2*t^7.227 + 2*t^7.279 + 2*t^7.331 + 4*t^7.383 + 2*t^7.435 + 2*t^7.487 + 3*t^7.539 + 3*t^7.591 + 3*t^7.643 + t^7.799 + t^7.851 + t^7.903 + t^8.402 + t^8.558 + 3*t^8.61 + 3*t^8.662 + 3*t^8.714 + 6*t^8.766 + 4*t^8.818 - 3*t^8.87 - 3*t^8.922 + t^8.974 - t^4.487/y - t^7.357/y - t^7.409/y + t^7.461/y - t^7.513/y + t^7.565/y + t^7.617/y + t^8.74/y + (4*t^8.792)/y + t^8.844/y + (4*t^8.896)/y + (4*t^8.948)/y - t^4.487*y - t^7.357*y - t^7.409*y + t^7.461*y - t^7.513*y + t^7.565*y + t^7.617*y + t^8.74*y + 4*t^8.792*y + t^8.844*y + 4*t^8.896*y + 4*t^8.948*y | (2*t^2.87)/g1^10 + (2*t^2.922)/g1^6 + 2*g1^2*t^3.026 + g1^14*t^3.182 + t^4.201/g1^23 + t^4.357/g1^11 + t^4.409/g1^7 + t^4.461/g1^3 + g1*t^4.513 + g1^5*t^4.565 + 2*g1^9*t^4.617 + g1^13*t^4.669 + g1^17*t^4.721 + (2*t^5.74)/g1^20 + (3*t^5.792)/g1^16 + (2*t^5.844)/g1^12 + (3*t^5.896)/g1^8 + (2*t^5.948)/g1^4 - 4*t^6. + 2*g1^4*t^6.052 + g1^8*t^6.104 - g1^12*t^6.156 + g1^16*t^6.208 - g1^20*t^6.26 + g1^28*t^6.364 + (2*t^7.071)/g1^33 + (2*t^7.123)/g1^29 + (2*t^7.227)/g1^21 + (2*t^7.279)/g1^17 + (2*t^7.331)/g1^13 + (4*t^7.383)/g1^9 + (2*t^7.435)/g1^5 + (2*t^7.487)/g1 + 3*g1^3*t^7.539 + 3*g1^7*t^7.591 + 3*g1^11*t^7.643 + g1^23*t^7.799 + g1^27*t^7.851 + g1^31*t^7.903 + t^8.402/g1^46 + t^8.558/g1^34 + (3*t^8.61)/g1^30 + (3*t^8.662)/g1^26 + (3*t^8.714)/g1^22 + (6*t^8.766)/g1^18 + (4*t^8.818)/g1^14 - (3*t^8.87)/g1^10 - (3*t^8.922)/g1^6 + t^8.974/g1^2 - t^4.487/(g1*y) - t^7.357/(g1^11*y) - t^7.409/(g1^7*y) + t^7.461/(g1^3*y) - (g1*t^7.513)/y + (g1^5*t^7.565)/y + (g1^9*t^7.617)/y + t^8.74/(g1^20*y) + (4*t^8.792)/(g1^16*y) + t^8.844/(g1^12*y) + (4*t^8.896)/(g1^8*y) + (4*t^8.948)/(g1^4*y) - (t^4.487*y)/g1 - (t^7.357*y)/g1^11 - (t^7.409*y)/g1^7 + (t^7.461*y)/g1^3 - g1*t^7.513*y + g1^5*t^7.565*y + g1^9*t^7.617*y + (t^8.74*y)/g1^20 + (4*t^8.792*y)/g1^16 + (t^8.844*y)/g1^12 + (4*t^8.896*y)/g1^8 + (4*t^8.948*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 56886 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6922 | 0.8481 | 0.8162 | [M:[1.0199, 0.9881, 0.9801, 1.004, 1.0119, 0.9881, 1.004], q:[0.502, 0.4781], qb:[0.5099, 0.5179], phi:[0.498]] | t^2.94 + 2*t^2.964 + 2*t^3.012 + t^3.06 + t^3.083 + t^4.363 + t^4.434 + t^4.458 + t^4.482 + t^4.506 + t^4.53 + 2*t^4.554 + t^4.577 + t^4.601 + t^5.905 + 2*t^5.928 + t^5.952 + 2*t^5.976 - 3*t^6. - t^4.494/y - t^4.494*y | detail |