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 |
|---|---|---|---|---|---|---|---|---|---|
| 1325 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}^{2}$ + ${ }M_{6}M_{7}$ | 0.7139 | 0.8726 | 0.8181 | [M:[1.0, 1.0786, 0.8428, 0.9943, 0.8485, 1.0057, 0.9943], q:[0.5057, 0.4943], qb:[0.5, 0.6572], phi:[0.4607]] | [M:[[0, 0], [0, 2], [0, -4], [1, 0], [-1, -4], [-1, 0], [1, 0]], q:[[-1, 0], [1, 0]], qb:[[0, 0], [0, 4]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{3}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$ | ${}$ | -3 | t^2.528 + t^2.545 + 2*t^2.983 + t^3. + t^3.236 + t^3.489 + t^4.348 + t^4.365 + 2*t^4.382 + t^4.399 + t^4.416 + t^4.837 + t^4.854 + t^4.871 + t^5.057 + t^5.074 + t^5.091 + t^5.326 + t^5.511 + 2*t^5.528 + t^5.764 + t^5.781 + 2*t^5.966 - 3*t^6. - t^6.017 + 2*t^6.219 + t^6.236 - t^6.455 + t^6.472 + t^6.725 + t^6.876 + t^6.893 + 2*t^6.91 + 2*t^6.928 + 2*t^6.945 + t^6.962 + t^6.978 + 2*t^7.33 + 2*t^7.348 + 3*t^7.365 + 2*t^7.382 + 2*t^7.399 + t^7.416 + t^7.585 + t^7.602 + t^7.619 + t^7.636 + t^7.819 + t^7.837 + t^7.854 + t^7.871 + t^7.905 + t^8.039 + 2*t^8.057 + t^8.074 + t^8.292 + t^8.308 + t^8.31 + t^8.326 + t^8.327 + t^8.36 - 4*t^8.528 - 4*t^8.545 - 2*t^8.563 + t^8.695 + t^8.713 + 2*t^8.73 + 3*t^8.747 + 5*t^8.764 + 2*t^8.781 + 2*t^8.799 + t^8.814 + t^8.816 + t^8.833 + 2*t^8.948 - t^8.966 - 7*t^8.983 - t^4.382/y - t^6.91/y - t^6.928/y - t^7.365/y + t^7.399/y + t^7.837/y + t^7.854/y + t^8.074/y + (2*t^8.511)/y + (3*t^8.528)/y + t^8.545/y + t^8.764/y + t^8.781/y + t^8.966/y + (2*t^8.983)/y - t^4.382*y - t^6.91*y - t^6.928*y - t^7.365*y + t^7.399*y + t^7.837*y + t^7.854*y + t^8.074*y + 2*t^8.511*y + 3*t^8.528*y + t^8.545*y + t^8.764*y + t^8.781*y + t^8.966*y + 2*t^8.983*y | t^2.528/g2^4 + t^2.545/(g1*g2^4) + 2*g1*t^2.983 + t^3. + g2^2*t^3.236 + (g2^4*t^3.489)/g1 + (g1^2*t^4.348)/g2 + (g1*t^4.365)/g2 + (2*t^4.382)/g2 + t^4.399/(g1*g2) + t^4.416/(g1^2*g2) + g1*g2^3*t^4.837 + g2^3*t^4.854 + (g2^3*t^4.871)/g1 + t^5.057/g2^8 + t^5.074/(g1*g2^8) + t^5.091/(g1^2*g2^8) + g2^7*t^5.326 + (g1*t^5.511)/g2^4 + (2*t^5.528)/g2^4 + t^5.764/g2^2 + t^5.781/(g1*g2^2) + 2*g1^2*t^5.966 - 3*t^6. - t^6.017/g1 + 2*g1*g2^2*t^6.219 + g2^2*t^6.236 - g1*g2^4*t^6.455 + g2^4*t^6.472 + (g2^6*t^6.725)/g1 + (g1^2*t^6.876)/g2^5 + (g1*t^6.893)/g2^5 + (2*t^6.91)/g2^5 + (2*t^6.928)/(g1*g2^5) + (2*t^6.945)/(g1^2*g2^5) + t^6.962/(g1^3*g2^5) + (g2^8*t^6.978)/g1^2 + (2*g1^3*t^7.33)/g2 + (2*g1^2*t^7.348)/g2 + (3*g1*t^7.365)/g2 + (2*t^7.382)/g2 + (2*t^7.399)/(g1*g2) + t^7.416/(g1^2*g2) + t^7.585/g2^12 + t^7.602/(g1*g2^12) + t^7.619/(g1^2*g2^12) + t^7.636/(g1^3*g2^12) + g1^2*g2^3*t^7.819 + g1*g2^3*t^7.837 + g2^3*t^7.854 + (g2^3*t^7.871)/g1 + (g2^3*t^7.905)/g1^3 + (g1*t^8.039)/g2^8 + (2*t^8.057)/g2^8 + t^8.074/(g1*g2^8) + t^8.292/g2^6 + g1*g2^7*t^8.308 + t^8.31/(g1*g2^6) + g2^7*t^8.326 + t^8.327/(g1^2*g2^6) + (g2^7*t^8.36)/g1^2 - (4*t^8.528)/g2^4 - (4*t^8.545)/(g1*g2^4) - (2*t^8.563)/(g1^2*g2^4) + (g1^4*t^8.695)/g2^2 + (g1^3*t^8.713)/g2^2 + (2*g1^2*t^8.73)/g2^2 + (3*g1*t^8.747)/g2^2 + (5*t^8.764)/g2^2 + (2*t^8.781)/(g1*g2^2) + (2*t^8.799)/(g1^2*g2^2) + (g2^11*t^8.814)/g1 + t^8.816/(g1^3*g2^2) + t^8.833/(g1^4*g2^2) + 2*g1^3*t^8.948 - g1^2*t^8.966 - 7*g1*t^8.983 - t^4.382/(g2*y) - t^6.91/(g2^5*y) - t^6.928/(g1*g2^5*y) - (g1*t^7.365)/(g2*y) + t^7.399/(g1*g2*y) + (g1*g2^3*t^7.837)/y + (g2^3*t^7.854)/y + t^8.074/(g1*g2^8*y) + (2*g1*t^8.511)/(g2^4*y) + (3*t^8.528)/(g2^4*y) + t^8.545/(g1*g2^4*y) + t^8.764/(g2^2*y) + t^8.781/(g1*g2^2*y) + (g1^2*t^8.966)/y + (2*g1*t^8.983)/y - (t^4.382*y)/g2 - (t^6.91*y)/g2^5 - (t^6.928*y)/(g1*g2^5) - (g1*t^7.365*y)/g2 + (t^7.399*y)/(g1*g2) + g1*g2^3*t^7.837*y + g2^3*t^7.854*y + (t^8.074*y)/(g1*g2^8) + (2*g1*t^8.511*y)/g2^4 + (3*t^8.528*y)/g2^4 + (t^8.545*y)/(g1*g2^4) + (t^8.764*y)/g2^2 + (t^8.781*y)/(g1*g2^2) + g1^2*t^8.966*y + 2*g1*t^8.983*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 |
|---|---|---|---|---|---|---|---|---|---|
| 834 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}^{2}$ | 0.7146 | 0.8745 | 0.8171 | [M:[1.0, 1.0767, 0.8466, 1.0202, 0.8264, 0.9798], q:[0.4798, 0.5202], qb:[0.5, 0.6534], phi:[0.4617]] | t^2.479 + t^2.54 + t^2.939 + t^3. + t^3.061 + t^3.23 + t^3.399 + t^4.264 + t^4.324 + 2*t^4.385 + t^4.446 + t^4.506 + t^4.784 + t^4.845 + t^4.906 + t^4.958 + t^5.019 + t^5.08 + t^5.305 + t^5.418 + t^5.479 + t^5.54 + t^5.709 + t^5.77 + t^5.879 - 2*t^6. - t^4.385/y - t^4.385*y | detail |