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 |
|---|---|---|---|---|---|---|---|---|---|
| 1428 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ | 0.6989 | 0.8581 | 0.8144 | [M:[0.9422, 1.0193, 1.0578, 0.9037, 1.0, 0.9807], q:[0.5, 0.5578], qb:[0.4422, 0.5385], phi:[0.4904]] | [M:[[-6], [2], [6], [-10], [0], [-2]], q:[[0], [6]], qb:[[-6], [4]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -2 | t^2.711 + t^2.827 + 2*t^2.942 + t^3. + t^3.116 + t^3.173 + t^4.124 + t^4.298 + t^4.413 + 2*t^4.471 + t^4.587 + t^4.644 + t^4.702 + t^4.76 + t^4.818 + t^5.422 + t^5.538 + 2*t^5.653 + 2*t^5.769 + 3*t^5.884 + 2*t^5.942 - 2*t^6. + t^6.058 + t^6.116 - t^6.173 + t^6.231 + t^6.835 + t^6.951 + t^7.009 + 2*t^7.067 + 2*t^7.124 + 3*t^7.24 + 2*t^7.298 + t^7.356 + 5*t^7.413 + t^7.529 + 3*t^7.587 + 2*t^7.644 + 2*t^7.702 + t^7.76 + t^7.818 + t^7.933 + t^7.991 + t^8.133 + 2*t^8.249 + 2*t^8.364 + t^8.422 + 2*t^8.48 + 5*t^8.595 - t^8.653 + t^8.711 + 2*t^8.769 + 3*t^8.884 - 3*t^8.942 - t^4.471/y - t^7.182/y - t^7.413/y + t^7.529/y + t^7.76/y + t^8.538/y + (2*t^8.653)/y + t^8.711/y + (2*t^8.769)/y + (2*t^8.827)/y + (2*t^8.884)/y + (3*t^8.942)/y - t^4.471*y - t^7.182*y - t^7.413*y + t^7.529*y + t^7.76*y + t^8.538*y + 2*t^8.653*y + t^8.711*y + 2*t^8.769*y + 2*t^8.827*y + 2*t^8.884*y + 3*t^8.942*y | t^2.711/g1^10 + t^2.827/g1^6 + (2*t^2.942)/g1^2 + t^3. + g1^4*t^3.116 + g1^6*t^3.173 + t^4.124/g1^13 + t^4.298/g1^7 + t^4.413/g1^3 + (2*t^4.471)/g1 + g1^3*t^4.587 + g1^5*t^4.644 + g1^7*t^4.702 + g1^9*t^4.76 + g1^11*t^4.818 + t^5.422/g1^20 + t^5.538/g1^16 + (2*t^5.653)/g1^12 + (2*t^5.769)/g1^8 + (3*t^5.884)/g1^4 + (2*t^5.942)/g1^2 - 2*t^6. + g1^2*t^6.058 + g1^4*t^6.116 - g1^6*t^6.173 + g1^8*t^6.231 + t^6.835/g1^23 + t^6.951/g1^19 + t^7.009/g1^17 + (2*t^7.067)/g1^15 + (2*t^7.124)/g1^13 + (3*t^7.24)/g1^9 + (2*t^7.298)/g1^7 + t^7.356/g1^5 + (5*t^7.413)/g1^3 + g1*t^7.529 + 3*g1^3*t^7.587 + 2*g1^5*t^7.644 + 2*g1^7*t^7.702 + g1^9*t^7.76 + g1^11*t^7.818 + g1^15*t^7.933 + g1^17*t^7.991 + t^8.133/g1^30 + (2*t^8.249)/g1^26 + (2*t^8.364)/g1^22 + t^8.422/g1^20 + (2*t^8.48)/g1^18 + (5*t^8.595)/g1^14 - t^8.653/g1^12 + t^8.711/g1^10 + (2*t^8.769)/g1^8 + (3*t^8.884)/g1^4 - (3*t^8.942)/g1^2 - t^4.471/(g1*y) - t^7.182/(g1^11*y) - t^7.413/(g1^3*y) + (g1*t^7.529)/y + (g1^9*t^7.76)/y + t^8.538/(g1^16*y) + (2*t^8.653)/(g1^12*y) + t^8.711/(g1^10*y) + (2*t^8.769)/(g1^8*y) + (2*t^8.827)/(g1^6*y) + (2*t^8.884)/(g1^4*y) + (3*t^8.942)/(g1^2*y) - (t^4.471*y)/g1 - (t^7.182*y)/g1^11 - (t^7.413*y)/g1^3 + g1*t^7.529*y + g1^9*t^7.76*y + (t^8.538*y)/g1^16 + (2*t^8.653*y)/g1^12 + (t^8.711*y)/g1^10 + (2*t^8.769*y)/g1^8 + (2*t^8.827*y)/g1^6 + (2*t^8.884*y)/g1^4 + (3*t^8.942*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 |
|---|---|---|---|---|---|---|---|---|---|
| 930 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.6972 | 0.855 | 0.8154 | [M:[0.949, 1.017, 1.051, 0.915, 1.0], q:[0.5, 0.551], qb:[0.449, 0.534], phi:[0.4915]] | t^2.745 + t^2.847 + t^2.949 + t^3. + t^3.051 + t^3.102 + t^3.153 + t^4.169 + t^4.322 + t^4.424 + 2*t^4.475 + t^4.576 + t^4.627 + t^4.678 + t^4.729 + t^4.78 + t^5.49 + t^5.592 + t^5.694 + 2*t^5.796 + 2*t^5.898 + t^5.949 - t^6. - t^4.475/y - t^4.475*y | detail |