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 |
---|
# | 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 |
---|---|---|---|---|---|---|---|---|---|
640 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6337 | 0.8024 | 0.7897 | [M:[1.2, 1.1, 0.7, 0.8], q:[0.75, 0.45], qb:[0.35, 0.45], phi:[0.5]] | [M:[[0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 20277/32000, c: 25677/32000, M1: 6/5, M2: 11/10, M3: 7/10, M4: 4/5, q1: 3/4, q2: 9/20, qb1: 7/20, qb2: 9/20, phi1: 1/2} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | ${}M_{4}q_{1}q_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 2 | t^2.1 + 2*t^2.4 + t^3. + 2*t^3.3 + 3*t^3.6 + t^3.9 + 4*t^4.2 + 2*t^4.5 + 3*t^4.8 + t^5.1 + 4*t^5.4 + 5*t^5.7 + 2*t^6. + 4*t^6.3 + 9*t^6.6 + 6*t^6.9 + 8*t^7.2 + 5*t^7.5 + 10*t^7.8 + 3*t^8.1 + 8*t^8.4 + 6*t^8.7 - t^4.5/y - t^6.6/y + t^7.2/y + (2*t^7.5)/y + t^8.1/y + (5*t^8.4)/y + (6*t^8.7)/y - t^4.5*y - t^6.6*y + t^7.2*y + 2*t^7.5*y + t^8.1*y + 5*t^8.4*y + 6*t^8.7*y | t^2.1 + 2*t^2.4 + t^3. + 2*t^3.3 + 3*t^3.6 + t^3.9 + 4*t^4.2 + 2*t^4.5 + 3*t^4.8 + t^5.1 + 4*t^5.4 + 5*t^5.7 + 2*t^6. + 4*t^6.3 + 9*t^6.6 + 6*t^6.9 + 8*t^7.2 + 5*t^7.5 + 10*t^7.8 + 3*t^8.1 + 8*t^8.4 + 6*t^8.7 - t^4.5/y - t^6.6/y + t^7.2/y + (2*t^7.5)/y + t^8.1/y + (5*t^8.4)/y + (6*t^8.7)/y - t^4.5*y - t^6.6*y + t^7.2*y + 2*t^7.5*y + t^8.1*y + 5*t^8.4*y + 6*t^8.7*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 |
---|
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|
1020 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ | 0.6502 | 0.8314 | 0.782 | [M:[1.2, 1.1, 0.7, 0.8, 0.8], q:[0.75, 0.45], qb:[0.35, 0.45], phi:[0.5]] | t^2.1 + 3*t^2.4 + t^3. + 2*t^3.3 + 2*t^3.6 + t^3.9 + 4*t^4.2 + 3*t^4.5 + 6*t^4.8 + t^5.1 + 5*t^5.4 + 6*t^5.7 + 2*t^6. - t^4.5/y - t^4.5*y | detail | {a: 4161/6400, c: 5321/6400, M1: 6/5, M2: 11/10, M3: 7/10, M4: 4/5, M5: 4/5, q1: 3/4, q2: 9/20, qb1: 7/20, qb2: 9/20, phi1: 1/2} |
1019 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ | 0.6428 | 0.8178 | 0.786 | [M:[1.2, 1.1, 0.7, 0.8, 0.9], q:[0.75, 0.45], qb:[0.35, 0.45], phi:[0.5]] | t^2.1 + 2*t^2.4 + t^2.7 + t^3. + t^3.3 + 3*t^3.6 + t^3.9 + 4*t^4.2 + 2*t^4.5 + 4*t^4.8 + 3*t^5.1 + 4*t^5.4 + 4*t^5.7 + 3*t^6. - t^4.5/y - t^4.5*y | detail | {a: 2571/4000, c: 3271/4000, M1: 6/5, M2: 11/10, M3: 7/10, M4: 4/5, M5: 9/10, q1: 3/4, q2: 9/20, qb1: 7/20, qb2: 9/20, phi1: 1/2} |
1018 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ | 0.6131 | 0.7631 | 0.8034 | [M:[1.2, 1.1, 0.7, 0.8, 1.3], q:[0.75, 0.45], qb:[0.35, 0.45], phi:[0.5]] | 2*t^2.4 + t^3. + 2*t^3.3 + 3*t^3.6 + 2*t^3.9 + 3*t^4.2 + 3*t^4.8 + 2*t^5.4 + 2*t^5.7 + t^6. - t^4.5/y - t^4.5*y | detail | {a: 981/1600, c: 1221/1600, M1: 6/5, M2: 11/10, M3: 7/10, M4: 4/5, M5: 13/10, q1: 3/4, q2: 9/20, qb1: 7/20, qb2: 9/20, phi1: 1/2} |
1022 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6542 | 0.8417 | 0.7772 | [M:[1.2, 1.1, 0.7, 0.8, 0.7], q:[0.75, 0.45], qb:[0.35, 0.45], phi:[0.5]] | 2*t^2.1 + 2*t^2.4 + t^3. + 2*t^3.3 + 3*t^3.6 + 6*t^4.2 + 4*t^4.5 + 3*t^4.8 + 2*t^5.1 + 6*t^5.4 + 8*t^5.7 + t^6. - t^4.5/y - t^4.5*y | detail | {a: 10467/16000, c: 13467/16000, M1: 6/5, M2: 11/10, M3: 7/10, M4: 4/5, M5: 7/10, q1: 3/4, q2: 9/20, qb1: 7/20, qb2: 9/20, phi1: 1/2} |
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 |
---|
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
No data available in table |
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 |
---|
Loading... |
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 |
---|
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
398 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ | 0.6341 | 0.8036 | 0.7891 | [M:[1.211, 1.1055, 0.6835, 0.789], q:[0.75, 0.4335], qb:[0.3555, 0.461], phi:[0.5]] | t^2.05 + t^2.367 + t^2.45 + t^3. + 2*t^3.317 + t^3.55 + 2*t^3.633 + t^3.867 + 2*t^4.101 + t^4.183 + t^4.266 + t^4.417 + t^4.5 + t^4.734 + t^4.817 + t^4.899 + t^5.05 + 3*t^5.367 + t^5.45 + t^5.601 + 3*t^5.683 + t^5.766 + t^5.917 - t^4.5/y - t^4.5*y | detail |