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 |
|---|---|---|---|---|---|---|---|---|---|
| 57697 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{3}$ + ${ }M_{2}M_{7}$ | 0.7022 | 0.8641 | 0.8127 | [M:[1.051, 1.051, 0.949, 0.8979, 1.0, 0.949, 0.949], q:[0.449, 0.5], qb:[0.5, 0.6021], phi:[0.4872]] | [M:[[4], [4], [-4], [-8], [0], [-4], [-4]], q:[[-4], [0]], qb:[[0], [8]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | -4 | t^2.694 + 3*t^2.847 + t^2.923 + t^3. + t^3.306 + t^4.156 + 2*t^4.309 + 3*t^4.462 + t^4.615 + 2*t^4.768 + t^5.074 + t^5.388 + 2*t^5.541 + t^5.617 + 5*t^5.694 + 3*t^5.77 + 2*t^5.847 + t^5.923 - 4*t^6. + t^6.23 - t^6.306 - t^6.459 + t^6.612 + t^6.849 + 4*t^7.002 + t^7.079 + 7*t^7.156 + t^7.232 + 8*t^7.309 + t^7.385 + 2*t^7.462 - 2*t^7.538 + 2*t^7.615 + t^7.691 + 2*t^7.768 - 2*t^7.844 + t^7.921 + t^7.998 + 2*t^8.074 + t^8.082 - t^8.151 + 2*t^8.235 + 2*t^8.311 + t^8.38 + 3*t^8.388 + 4*t^8.464 + 6*t^8.541 + 8*t^8.617 - t^8.694 + 7*t^8.77 - 14*t^8.847 + 3*t^8.923 - t^4.462/y - t^7.156/y - t^7.309/y - t^7.385/y + t^7.538/y + t^7.615/y + t^7.768/y + (3*t^8.541)/y + t^8.617/y + (4*t^8.694)/y + (3*t^8.77)/y + (3*t^8.847)/y + t^8.923/y - t^4.462*y - t^7.156*y - t^7.309*y - t^7.385*y + t^7.538*y + t^7.615*y + t^7.768*y + 3*t^8.541*y + t^8.617*y + 4*t^8.694*y + 3*t^8.77*y + 3*t^8.847*y + t^8.923*y | t^2.694/g1^8 + (3*t^2.847)/g1^4 + t^2.923/g1^2 + t^3. + g1^8*t^3.306 + t^4.156/g1^9 + (2*t^4.309)/g1^5 + (3*t^4.462)/g1 + g1^3*t^4.615 + 2*g1^7*t^4.768 + g1^15*t^5.074 + t^5.388/g1^16 + (2*t^5.541)/g1^12 + t^5.617/g1^10 + (5*t^5.694)/g1^8 + (3*t^5.77)/g1^6 + (2*t^5.847)/g1^4 + t^5.923/g1^2 - 4*t^6. + g1^6*t^6.23 - g1^8*t^6.306 - g1^12*t^6.459 + g1^16*t^6.612 + t^6.849/g1^17 + (4*t^7.002)/g1^13 + t^7.079/g1^11 + (7*t^7.156)/g1^9 + t^7.232/g1^7 + (8*t^7.309)/g1^5 + t^7.385/g1^3 + (2*t^7.462)/g1 - 2*g1*t^7.538 + 2*g1^3*t^7.615 + g1^5*t^7.691 + 2*g1^7*t^7.768 - 2*g1^9*t^7.844 + g1^11*t^7.921 + g1^13*t^7.998 + 2*g1^15*t^8.074 + t^8.082/g1^24 - g1^17*t^8.151 + (2*t^8.235)/g1^20 + (2*t^8.311)/g1^18 + g1^23*t^8.38 + (3*t^8.388)/g1^16 + (4*t^8.464)/g1^14 + (6*t^8.541)/g1^12 + (8*t^8.617)/g1^10 - t^8.694/g1^8 + (7*t^8.77)/g1^6 - (14*t^8.847)/g1^4 + (3*t^8.923)/g1^2 - t^4.462/(g1*y) - t^7.156/(g1^9*y) - t^7.309/(g1^5*y) - t^7.385/(g1^3*y) + (g1*t^7.538)/y + (g1^3*t^7.615)/y + (g1^7*t^7.768)/y + (3*t^8.541)/(g1^12*y) + t^8.617/(g1^10*y) + (4*t^8.694)/(g1^8*y) + (3*t^8.77)/(g1^6*y) + (3*t^8.847)/(g1^4*y) + t^8.923/(g1^2*y) - (t^4.462*y)/g1 - (t^7.156*y)/g1^9 - (t^7.309*y)/g1^5 - (t^7.385*y)/g1^3 + g1*t^7.538*y + g1^3*t^7.615*y + g1^7*t^7.768*y + (3*t^8.541*y)/g1^12 + (t^8.617*y)/g1^10 + (4*t^8.694*y)/g1^8 + (3*t^8.77*y)/g1^6 + (3*t^8.847*y)/g1^4 + (t^8.923*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55955 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{3}$ | 0.698 | 0.8561 | 0.8153 | [M:[1.0398, 1.0398, 0.9602, 0.9204, 1.0, 0.9602], q:[0.4602, 0.5], qb:[0.5, 0.5796], phi:[0.4901]] | t^2.761 + 2*t^2.881 + t^2.94 + t^3. + t^3.119 + t^3.239 + t^4.231 + 2*t^4.351 + 3*t^4.47 + t^4.59 + 2*t^4.709 + t^4.948 + t^5.523 + t^5.642 + t^5.702 + 2*t^5.761 + 2*t^5.821 + 2*t^5.881 + t^5.94 - 2*t^6. - t^4.47/y - t^4.47*y | detail |