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 |
|---|---|---|---|---|---|---|---|---|---|
| 1196 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{2}^{2}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{3}M_{6}$ | 0.713 | 0.8864 | 0.8043 | [M:[0.9696, 1.0, 1.0304, 0.7143, 0.6839, 0.9696], q:[0.7857, 0.5304], qb:[0.5, 0.4696], phi:[0.4286]] | [M:[[1], [0], [-1], [0], [1], [1]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.052 + t^2.143 + t^2.571 + 2*t^2.909 + t^3. + t^3.766 + 2*t^4.104 + 2*t^4.195 + 3*t^4.286 + t^4.377 + t^4.468 + t^4.623 + t^4.714 + 2*t^4.961 + 3*t^5.052 + 2*t^5.143 + 2*t^5.48 + t^5.571 + 3*t^5.818 + t^5.909 - 2*t^6. - 2*t^6.091 + 2*t^6.155 - t^6.182 + 3*t^6.246 + 4*t^6.338 + 3*t^6.429 + t^6.52 + t^6.611 + 4*t^6.675 + 2*t^6.766 + t^6.857 + 4*t^7.013 + t^7.039 + 5*t^7.104 + 6*t^7.195 + 3*t^7.286 + 2*t^7.532 + 2*t^7.623 - t^7.805 + 4*t^7.87 - t^7.896 + 3*t^7.961 + t^8.052 - 4*t^8.143 + 3*t^8.207 - 4*t^8.234 + 4*t^8.298 - 2*t^8.325 + 9*t^8.389 + 5*t^8.48 + 3*t^8.571 + 6*t^8.727 + 2*t^8.754 + 4*t^8.818 + t^8.845 - 3*t^8.909 + t^8.936 - t^4.286/y - t^6.338/y - t^6.429/y - t^6.857/y + t^7.377/y + t^7.623/y + (2*t^7.714)/y + (2*t^7.961)/y + (3*t^8.052)/y + (2*t^8.143)/y + t^8.234/y - t^8.389/y + t^8.48/y + (2*t^8.818)/y + (2*t^8.909)/y - t^4.286*y - t^6.338*y - t^6.429*y - t^6.857*y + t^7.377*y + t^7.623*y + 2*t^7.714*y + 2*t^7.961*y + 3*t^8.052*y + 2*t^8.143*y + t^8.234*y - t^8.389*y + t^8.48*y + 2*t^8.818*y + 2*t^8.909*y | g1*t^2.052 + t^2.143 + t^2.571 + 2*g1*t^2.909 + t^3. + g1*t^3.766 + 2*g1^2*t^4.104 + 2*g1*t^4.195 + 3*t^4.286 + t^4.377/g1 + t^4.468/g1^2 + g1*t^4.623 + t^4.714 + 2*g1^2*t^4.961 + 3*g1*t^5.052 + 2*t^5.143 + 2*g1*t^5.48 + t^5.571 + 3*g1^2*t^5.818 + g1*t^5.909 - 2*t^6. - (2*t^6.091)/g1 + 2*g1^3*t^6.155 - t^6.182/g1^2 + 3*g1^2*t^6.246 + 4*g1*t^6.338 + 3*t^6.429 + t^6.52/g1 + t^6.611/g1^2 + 4*g1^2*t^6.675 + 2*g1*t^6.766 + t^6.857 + 4*g1^3*t^7.013 + t^7.039/g1^2 + 5*g1^2*t^7.104 + 6*g1*t^7.195 + 3*t^7.286 + 2*g1^2*t^7.532 + 2*g1*t^7.623 - t^7.805/g1 + 4*g1^3*t^7.87 - t^7.896/g1^2 + 3*g1^2*t^7.961 + g1*t^8.052 - 4*t^8.143 + 3*g1^4*t^8.207 - (4*t^8.234)/g1 + 4*g1^3*t^8.298 - (2*t^8.325)/g1^2 + 9*g1^2*t^8.389 + 5*g1*t^8.48 + 3*t^8.571 + 6*g1^3*t^8.727 + (2*t^8.754)/g1^2 + 4*g1^2*t^8.818 + t^8.845/g1^3 - 3*g1*t^8.909 + t^8.936/g1^4 - t^4.286/y - (g1*t^6.338)/y - t^6.429/y - t^6.857/y + t^7.377/(g1*y) + (g1*t^7.623)/y + (2*t^7.714)/y + (2*g1^2*t^7.961)/y + (3*g1*t^8.052)/y + (2*t^8.143)/y + t^8.234/(g1*y) - (g1^2*t^8.389)/y + (g1*t^8.48)/y + (2*g1^2*t^8.818)/y + (2*g1*t^8.909)/y - t^4.286*y - g1*t^6.338*y - t^6.429*y - t^6.857*y + (t^7.377*y)/g1 + g1*t^7.623*y + 2*t^7.714*y + 2*g1^2*t^7.961*y + 3*g1*t^8.052*y + 2*t^8.143*y + (t^8.234*y)/g1 - g1^2*t^8.389*y + g1*t^8.48*y + 2*g1^2*t^8.818*y + 2*g1*t^8.909*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 728 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{2}^{2}$ + ${ }M_{5}q_{1}q_{2}$ | 0.7113 | 0.8813 | 0.8071 | [M:[0.9936, 1.0, 1.0064, 0.7143, 0.7078], q:[0.7857, 0.5064], qb:[0.5, 0.4936], phi:[0.4286]] | t^2.124 + t^2.143 + t^2.571 + t^2.981 + t^3. + t^3.019 + t^3.838 + 2*t^4.247 + 2*t^4.266 + 3*t^4.286 + t^4.305 + t^4.324 + t^4.695 + t^4.714 + t^5.104 + 2*t^5.124 + 3*t^5.143 + t^5.162 + t^5.552 + t^5.571 + t^5.591 + t^5.961 - t^6. - t^4.286/y - t^4.286*y | detail |