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 |
|---|---|---|---|---|---|---|---|---|---|
| 335 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 0.5742 | 0.7205 | 0.797 | [M:[1.0, 1.1067, 0.7865], q:[0.7767, 0.2233], qb:[0.6699, 0.5436], phi:[0.4466]] | [M:[[0], [4], [-8]], q:[[1], [-1]], qb:[[-3], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{2}q_{2}^{4}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -1 | t^2.301 + t^2.36 + 2*t^2.68 + t^3. + t^3.32 + t^3.64 + t^3.961 + t^4.02 + t^4.34 + 2*t^4.601 + t^4.719 + 3*t^4.98 + t^5.039 + t^5.301 + 5*t^5.36 + 2*t^5.68 + t^5.941 - t^6. + t^6.261 + 3*t^6.32 - t^6.379 + 2*t^6.64 + 2*t^6.699 + 2*t^6.902 + t^7.02 + t^7.079 + 5*t^7.281 - 2*t^7.34 + t^7.399 + 2*t^7.601 + 4*t^7.66 + 2*t^7.719 + t^7.921 + 2*t^7.98 + 7*t^8.039 + 2*t^8.242 - 3*t^8.301 + t^8.36 + 2*t^8.562 + 2*t^8.621 - 5*t^8.68 + 2*t^8.941 - t^4.34/y - t^6.699/y + t^7.66/y + (3*t^7.98)/y + (2*t^8.039)/y + t^8.301/y + (2*t^8.36)/y + t^8.621/y + (3*t^8.68)/y + t^8.941/y - t^4.34*y - t^6.699*y + t^7.66*y + 3*t^7.98*y + 2*t^8.039*y + t^8.301*y + 2*t^8.36*y + t^8.621*y + 3*t^8.68*y + t^8.941*y | g1^10*t^2.301 + t^2.36/g1^8 + (2*t^2.68)/g1^4 + t^3. + g1^4*t^3.32 + g1^8*t^3.64 + g1^12*t^3.961 + t^4.02/g1^6 + t^4.34/g1^2 + 2*g1^20*t^4.601 + t^4.719/g1^16 + 3*g1^6*t^4.98 + t^5.039/g1^12 + g1^10*t^5.301 + (5*t^5.36)/g1^8 + (2*t^5.68)/g1^4 + g1^18*t^5.941 - t^6. + g1^22*t^6.261 + 3*g1^4*t^6.32 - t^6.379/g1^14 + 2*g1^8*t^6.64 + (2*t^6.699)/g1^10 + 2*g1^30*t^6.902 + t^7.02/g1^6 + t^7.079/g1^24 + 5*g1^16*t^7.281 - (2*t^7.34)/g1^2 + t^7.399/g1^20 + 2*g1^20*t^7.601 + 4*g1^2*t^7.66 + (2*t^7.719)/g1^16 + g1^24*t^7.921 + 2*g1^6*t^7.98 + (7*t^8.039)/g1^12 + 2*g1^28*t^8.242 - 3*g1^10*t^8.301 + t^8.36/g1^8 + 2*g1^32*t^8.562 + 2*g1^14*t^8.621 - (5*t^8.68)/g1^4 + 2*g1^18*t^8.941 - t^4.34/(g1^2*y) - t^6.699/(g1^10*y) + (g1^2*t^7.66)/y + (3*g1^6*t^7.98)/y + (2*t^8.039)/(g1^12*y) + (g1^10*t^8.301)/y + (2*t^8.36)/(g1^8*y) + (g1^14*t^8.621)/y + (3*t^8.68)/(g1^4*y) + (g1^18*t^8.941)/y - (t^4.34*y)/g1^2 - (t^6.699*y)/g1^10 + g1^2*t^7.66*y + 3*g1^6*t^7.98*y + (2*t^8.039*y)/g1^12 + g1^10*t^8.301*y + (2*t^8.36*y)/g1^8 + g1^14*t^8.621*y + (3*t^8.68*y)/g1^4 + g1^18*t^8.941*y |
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 |
|---|---|---|---|---|---|---|---|---|
| 529 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | 0.5741 | 0.7199 | 0.7974 | [M:[1.0, 1.1111, 0.7778], q:[0.7778, 0.2222], qb:[0.6667, 0.5556], phi:[0.4444]] | 2*t^2.333 + 2*t^2.667 + t^3. + t^3.333 + t^3.667 + 2*t^4. + t^4.333 + 3*t^4.667 + 4*t^5. + 6*t^5.333 + 2*t^5.667 - t^4.333/y - t^4.333*y | detail | {a: 31/54, c: 311/432, M1: 1, M2: 10/9, M3: 7/9, q1: 7/9, q2: 2/9, qb1: 2/3, qb2: 5/9, phi1: 4/9} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 208 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ | 0.5895 | 0.742 | 0.7945 | [M:[1.0, 1.0406, 0.9189], q:[0.7601, 0.2399], qb:[0.5406, 0.5406], phi:[0.4797]] | 2*t^2.341 + t^2.757 + t^2.878 + t^3. + t^3.122 + 2*t^3.78 + 2*t^3.902 + 6*t^4.683 + 2*t^5.22 + 2*t^5.341 + 2*t^5.463 + t^5.513 + t^5.635 + 2*t^5.757 + t^5.878 - 4*t^6. - t^4.439/y - t^4.439*y | detail |