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 |
|---|---|---|---|---|---|---|---|---|---|
| 1508 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}M_{6}$ | 0.7026 | 0.8635 | 0.8137 | [M:[1.0, 0.9408, 1.0592, 0.8817, 1.0296, 0.9408], q:[0.4852, 0.5148], qb:[0.4556, 0.6035], phi:[0.4852]] | [M:[[0], [-4], [4], [-8], [2], [-4]], q:[[-1], [1]], qb:[[-3], [7]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.645 + 2*t^2.823 + t^2.911 + t^3. + t^3.089 + t^3.266 + t^4.189 + t^4.278 + 2*t^4.367 + t^4.456 + t^4.544 + t^4.633 + t^4.722 + t^4.811 + t^5.077 + t^5.29 + 2*t^5.468 + 3*t^5.645 + 2*t^5.734 + 2*t^5.823 + 2*t^5.911 - 2*t^6. + t^6.089 - t^6.444 + t^6.532 + t^6.835 + t^6.923 + 3*t^7.012 + 3*t^7.101 + 5*t^7.189 + 4*t^7.278 + 3*t^7.367 + 2*t^7.456 + t^7.544 + 2*t^7.633 + t^7.722 + t^7.899 + t^7.935 + t^7.988 + t^8.077 + 2*t^8.113 + 3*t^8.29 + t^8.343 + 2*t^8.379 + 4*t^8.468 + 4*t^8.556 + t^8.645 + 4*t^8.734 - 3*t^8.823 - t^4.456/y - t^7.101/y - t^7.278/y + t^7.633/y + t^7.811/y + (2*t^8.468)/y + t^8.556/y + (2*t^8.645)/y + (3*t^8.734)/y + (2*t^8.823)/y + (4*t^8.911)/y - t^4.456*y - t^7.101*y - t^7.278*y + t^7.633*y + t^7.811*y + 2*t^8.468*y + t^8.556*y + 2*t^8.645*y + 3*t^8.734*y + 2*t^8.823*y + 4*t^8.911*y | t^2.645/g1^8 + (2*t^2.823)/g1^4 + t^2.911/g1^2 + t^3. + g1^2*t^3.089 + g1^6*t^3.266 + t^4.189/g1^7 + t^4.278/g1^5 + (2*t^4.367)/g1^3 + t^4.456/g1 + g1*t^4.544 + g1^3*t^4.633 + g1^5*t^4.722 + g1^7*t^4.811 + g1^13*t^5.077 + t^5.29/g1^16 + (2*t^5.468)/g1^12 + (3*t^5.645)/g1^8 + (2*t^5.734)/g1^6 + (2*t^5.823)/g1^4 + (2*t^5.911)/g1^2 - 2*t^6. + g1^2*t^6.089 - g1^10*t^6.444 + g1^12*t^6.532 + t^6.835/g1^15 + t^6.923/g1^13 + (3*t^7.012)/g1^11 + (3*t^7.101)/g1^9 + (5*t^7.189)/g1^7 + (4*t^7.278)/g1^5 + (3*t^7.367)/g1^3 + (2*t^7.456)/g1 + g1*t^7.544 + 2*g1^3*t^7.633 + g1^5*t^7.722 + g1^9*t^7.899 + t^7.935/g1^24 + g1^11*t^7.988 + g1^13*t^8.077 + (2*t^8.113)/g1^20 + (3*t^8.29)/g1^16 + g1^19*t^8.343 + (2*t^8.379)/g1^14 + (4*t^8.468)/g1^12 + (4*t^8.556)/g1^10 + t^8.645/g1^8 + (4*t^8.734)/g1^6 - (3*t^8.823)/g1^4 - t^4.456/(g1*y) - t^7.101/(g1^9*y) - t^7.278/(g1^5*y) + (g1^3*t^7.633)/y + (g1^7*t^7.811)/y + (2*t^8.468)/(g1^12*y) + t^8.556/(g1^10*y) + (2*t^8.645)/(g1^8*y) + (3*t^8.734)/(g1^6*y) + (2*t^8.823)/(g1^4*y) + (4*t^8.911)/(g1^2*y) - (t^4.456*y)/g1 - (t^7.101*y)/g1^9 - (t^7.278*y)/g1^5 + g1^3*t^7.633*y + g1^7*t^7.811*y + (2*t^8.468*y)/g1^12 + (t^8.556*y)/g1^10 + (2*t^8.645*y)/g1^8 + (3*t^8.734*y)/g1^6 + (2*t^8.823*y)/g1^4 + (4*t^8.911*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 |
|---|---|---|---|---|---|---|---|---|---|
| 970 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ | 0.6978 | 0.8548 | 0.8164 | [M:[1.0, 0.9552, 1.0448, 0.9105, 1.0224], q:[0.4888, 0.5112], qb:[0.4664, 0.5784], phi:[0.4888]] | t^2.731 + t^2.866 + t^2.933 + t^3. + t^3.067 + t^3.134 + t^3.201 + t^4.265 + t^4.332 + 2*t^4.399 + t^4.466 + t^4.534 + t^4.601 + t^4.668 + t^4.735 + t^4.937 + t^5.463 + t^5.597 + t^5.731 + t^5.799 + 2*t^5.866 + t^5.933 - t^6. - t^4.466/y - t^4.466*y | detail |