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 |
|---|---|---|---|---|---|---|---|---|---|
| 2464 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{7}$ | 0.7262 | 0.9027 | 0.8045 | [M:[1.0, 0.8561, 1.0719, 0.7842, 1.0, 0.8561, 0.9281], q:[0.464, 0.536], qb:[0.464, 0.6798], phi:[0.464]] | [M:[[0], [-4], [2], [-6], [0], [-4], [-2]], q:[[-1], [1]], qb:[[-1], [5]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{1}M_{5}$ | -3 | t^2.353 + 2*t^2.568 + 2*t^2.784 + 2*t^3. + 3*t^4.176 + 2*t^4.392 + t^4.608 + t^4.705 + 2*t^4.824 + 2*t^4.921 + t^5.039 + 5*t^5.137 + 4*t^5.353 + t^5.471 + 6*t^5.568 + 2*t^5.784 - 3*t^6. - 2*t^6.216 - 2*t^6.432 + 3*t^6.529 - 2*t^6.647 + 6*t^6.745 + 10*t^6.961 + t^7.058 + 10*t^7.176 + 2*t^7.274 + 2*t^7.392 + 5*t^7.489 + 2*t^7.608 + 8*t^7.705 + 9*t^7.921 - 2*t^8.039 + 8*t^8.137 + 6*t^8.353 - 2*t^8.568 - t^8.687 - 11*t^8.784 + 3*t^8.882 - t^4.392/y - t^6.745/y - (2*t^6.961)/y - t^7.176/y + t^7.608/y + (2*t^7.824)/y + (2*t^7.921)/y + t^8.039/y + (3*t^8.137)/y + (6*t^8.353)/y + (5*t^8.568)/y + (4*t^8.784)/y - t^4.392*y - t^6.745*y - 2*t^6.961*y - t^7.176*y + t^7.608*y + 2*t^7.824*y + 2*t^7.921*y + t^8.039*y + 3*t^8.137*y + 6*t^8.353*y + 5*t^8.568*y + 4*t^8.784*y | t^2.353/g1^6 + (2*t^2.568)/g1^4 + (2*t^2.784)/g1^2 + 2*t^3. + (3*t^4.176)/g1^3 + (2*t^4.392)/g1 + g1*t^4.608 + t^4.705/g1^12 + 2*g1^3*t^4.824 + (2*t^4.921)/g1^10 + g1^5*t^5.039 + (5*t^5.137)/g1^8 + (4*t^5.353)/g1^6 + g1^9*t^5.471 + (6*t^5.568)/g1^4 + (2*t^5.784)/g1^2 - 3*t^6. - 2*g1^2*t^6.216 - 2*g1^4*t^6.432 + (3*t^6.529)/g1^9 - 2*g1^6*t^6.647 + (6*t^6.745)/g1^7 + (10*t^6.961)/g1^5 + t^7.058/g1^18 + (10*t^7.176)/g1^3 + (2*t^7.274)/g1^16 + (2*t^7.392)/g1 + (5*t^7.489)/g1^14 + 2*g1*t^7.608 + (8*t^7.705)/g1^12 + (9*t^7.921)/g1^10 - 2*g1^5*t^8.039 + (8*t^8.137)/g1^8 + (6*t^8.353)/g1^6 - (2*t^8.568)/g1^4 - g1^11*t^8.687 - (11*t^8.784)/g1^2 + (3*t^8.882)/g1^15 - t^4.392/(g1*y) - t^6.745/(g1^7*y) - (2*t^6.961)/(g1^5*y) - t^7.176/(g1^3*y) + (g1*t^7.608)/y + (2*g1^3*t^7.824)/y + (2*t^7.921)/(g1^10*y) + (g1^5*t^8.039)/y + (3*t^8.137)/(g1^8*y) + (6*t^8.353)/(g1^6*y) + (5*t^8.568)/(g1^4*y) + (4*t^8.784)/(g1^2*y) - (t^4.392*y)/g1 - (t^6.745*y)/g1^7 - (2*t^6.961*y)/g1^5 - (t^7.176*y)/g1^3 + g1*t^7.608*y + 2*g1^3*t^7.824*y + (2*t^7.921*y)/g1^10 + g1^5*t^8.039*y + (3*t^8.137*y)/g1^8 + (6*t^8.353*y)/g1^6 + (5*t^8.568*y)/g1^4 + (4*t^8.784*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1401 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.7198 | 0.8904 | 0.8084 | [M:[1.0, 0.8691, 1.0654, 0.8037, 1.0, 0.8691], q:[0.4673, 0.5327], qb:[0.4673, 0.6636], phi:[0.4673]] | t^2.411 + 2*t^2.607 + t^2.804 + 2*t^3. + t^3.196 + 3*t^4.206 + 2*t^4.402 + t^4.598 + 2*t^4.794 + t^4.822 + t^4.991 + 2*t^5.018 + 4*t^5.215 + t^5.383 + 2*t^5.411 + 5*t^5.607 + 2*t^5.804 - 2*t^6. - t^4.402/y - t^4.402*y | detail |